diff --git "a/1dAzT4oBgHgl3EQfDfo-/content/tmp_files/load_file.txt" "b/1dAzT4oBgHgl3EQfDfo-/content/tmp_files/load_file.txt" new file mode 100644--- /dev/null +++ "b/1dAzT4oBgHgl3EQfDfo-/content/tmp_files/load_file.txt" @@ -0,0 +1,962 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf,len=961 +page_content='arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='00976v1 [hep-ph] 3 Jan 2023 The Σ and Ξ electromagnetic form factors in the extended vector meson dominance model Bing Yan,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' ∗ Cheng Chen,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' † and Ju-Jun Xie2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 3,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 4,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' ‡ 1College of Mathematics and Physics,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chengdu University of Technology,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chengdu 610059,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' China 2Institute of Modern Physics,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chinese Academy of Sciences,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lanzhou 730000,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' China 3School of Nuclear Sciences and Technology,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' University of Chinese Academy of Sciences,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Beijing 101408,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' China 4Southern Center for Nuclear-Science Theory (SCNT),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Institute of Modern Physics,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chinese Academy of Sciences,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Huizhou 516000,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Guangdong Province,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' China We propose a phenomenological extended vector meson dominance model for the baryon electromagnetic structure,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' and it is found that the current experimental data on the Σ and Ξ electromagnetic form factors in the time-like region can be well described.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meanwhile, we can also reproduce the ratios of the total cross sections of reactions e+e− → Σ+ ¯Σ−, Σ0 ¯Σ0, and Σ− ¯Σ+, which are 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 ± 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 : 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 : 1 at center-of-mass energies from 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3864 to 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 GeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' We also analytically continue the expression of the form factors to space- like region and estimate the charge radii of the Σ and Ξ hyperons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The result for the Σ− is in agreement with the experimental date.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' INTRODUCTION The electromagnetic structure information of hadrons is characterized by the electromagnetic form factors (EMFFs), which are functions of the four-momentum transfer squared q2, with q the four-momentum carried by the exchanged vir- tual photon.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Study of these EMFFs can lead to a better under- standing of fundamental structure of hadrons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' On the experi- mental side, most commonly the baryon EMFFs in the space- like region (q2 < 0) were measured in the electron-baryon scattering [1–4].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' While for these unstable hadrons, for ex- ample, these hyperons, their EMFFs in the space-like region are very difficult to be experimentally measured.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' However, in the time-like region (q2 > 0), their EMFFs can be measured through the electron-positron annihilation reactions by the BESIII and Belle collaborations [5–12].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meanwhile, the ef- fective form factor Geff(q2) of hyperons can be extracted from the high-precision measured Born cross sections of the reac- tions e+e− → Y ¯Y (Y stands for hyperon;' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' ¯Y is anti-hyperon).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It was pointed out that these baryon EMFFs in the time-like region can be associated with the time evolution of the charge and magnetic distributions inside the baryon [13, 14].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The hyperon effective form factors Geff(q2) are the func- tions that parametrize the γY ¯Y vertex generated by the strong interaction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' While, the production vertex γY ¯Y is very poorly understood so far [15, 16].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The vector meson dominance (VMD) model is a very successful tool for studying the nu- cleon electromagnetic form factors, in both the space-like and time-like regions [17–19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Within a modified VMD model, the EMFFs of Λ hyperon were investigated in Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [20, 21].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' By considering the Y ¯Y final sate interactions, the EMFFs of hyperons in the time-like region have been studied in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [22].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It is worth to mention that the enhancement of the ∗Electronic address: yanbing@impcas.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ac.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='cn †Electronic address: chencheng22@mails.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ucas.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ac.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='cn ‡Electronic address: xiejujun@impcas.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ac.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='cn effective form factor of the Λ hyperon seen in the e+e− → Λ¯Λ reaction, was reproduced within the two above different calculations in Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [20, 21] and Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [22], respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In the vector meson dominance model for studying the electro- magnetic form factors of baryons, there is a phenomenological intrinsic form factor g(q2).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' From these studies of the nucleon and hyperon EMFFs [17–29], it is found that a better choice of g(q2) is the dipole form g(q2) = 1 (1 − γq2)2 , (1) with γ a free parameter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In the space-like region, the dipole form is consistent with the results obtained from perturbative quantum chromodynamics calculations [30, 31].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In the time- like region, it should be noticed that γ is a positive parameter, thus g(q2) will have a pole in the position γ = 1/q2, such pole could be restricted in the unphysical region, if γ satisfy γ > 1/(4m2 Y ) for hyperon Y .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' For a long time, the simple dipole form paremetrization is very useful for the discussion of different baryons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' For exam- ple, the dipole form of g(q2) can well describe the effective form factors of Λ [20, 21], Σ [32], and Ξ [27].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' While for the nucleon, a good general review is given in Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [33–36], both from the theoretical and from the experimental points of view.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' However, these determined values of γ for different ground state octet baryons with spin 1/2 are much different, even for the triplet Σ+, Σ− and Σ0 [32].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The determined values of γ, from previous works, for nucleon, Λ, Σ, and Ξ0 baryons are collected in Table I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Nevertheless, the VMD model and the parametrization of g(q2) can give a reasonable description of the experimental data on the baryon EMFFs at the considered energy region.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Various experimental and theoretical efforts have been con- tributed to the electromagnetic form factors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Very recently, the EMFFs of Σ+, Σ−, and Σ0 hyperons in the time-like region, have been measured with high-precision by the BESIII collab- oration through e+e− → Σ+ ¯Σ− [9], Σ− ¯Σ+ [9], and Σ0 ¯Σ0 reactions [10] at center-of-mass energies from 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3864 to 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 GeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The resulting ratios of total cross sections of these above 2 TABLE I: Values of γ (in GeV−2) for octet baryons used in previous works.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Proton ([17–19]) Neutron ([24–27]) Λ ([20]) Λ ([21]) γ 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='408 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='408 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='336 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='48 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='08 Σ+ ([32]) Σ− ([32]) Σ0 ([27]) Ξ0 ([27]) γ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='46 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='18 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='13 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='26 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='21 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 three reactions are 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 ± 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 : 1 : 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 [9, 37, 38], which disagree with various theoretical model predictions [39, 40].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' After the experimental measurements of e+e− → Σ+ ¯Σ− and Σ− ¯Σ+ [9], the effective form factors of Σ+ and Σ− were in- vestigated by using the VMD model [32], where the param- eter γ were taken with different values for Σ+ and Σ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [22], by considering the final state interactions of Y ¯Y , the energy dependence of the three reactions e+e− → Σ+ ¯Σ−, Σ0 ¯Σ0, and Σ− ¯Σ+ at low energies can be roughly reproduced, and it was found that there is a strong interplay between Σ+ ¯Σ−, Σ0 ¯Σ0, and Σ− ¯Σ+ channel in the near-threshold re- gion, caused by the Σ¯Σ final state interactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In the present work, we revisit the EMFFs at the time-like region of Σ and Ξ hyperons within an extended vector meson dominance model, where the affects of the isospin combinations from isovector ρ0 and isoscalar ω and φ mesons are taken into account.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Fur- thermore, we assume that the values of model parameter γ are same for Σ and Ξ hyperons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In addition, a vector meson with mass around 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 GeV was considered for the sake of bet- ter fitting the EMFFs of the Ξ0 and Ξ− hyperons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' We then progress to an analysis of the electromagnetic form factors in the space-like region and evaluate the electromagnetic radius of Σ hyperons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The theoretical result for the Σ− hyperon is in agreement with the experimental measurements.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' This article is organized as follows: in next section we will show the theo- retical formalism of the Σ and Ξ electromagnetic form factors in the VMD model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Numerical results about the effective form factors of Σ and Ξ and total cross sections of e+e− → Σ¯Σ and Ξ¯Ξ are shown in Sec.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' III, and a short summary is given in the final section.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' II.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' FORMALISM As already pointed out, as fixed-energy e+e− colliders, the EMFFs of hyperons in the time-like region was extracted from the data on the differential cross section of the process e+e− → Y ¯Y .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' For analysis the data, the BESIII Collaboration use the energy scan method [41–43], while the initial state radiation method was used by Belle Collaboration [12] and BABAR collaboration [44, 45].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Besides, the effective form factors Geff can be easily obtained from the data of the total cross sections.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The module squared of effective form factor |Geff|2 is a linear combination of |GE|2 and |GM|2, and pro- portional to the total cross section of e+e− → Y ¯Y reaction.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In this work, we study the EMFFs of Σ and Ξ baryons in the time-like region with the experimental measurements on the e+e− → Y ¯Y reactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Based on parity conservation and Lorentz invariant, the electromagnetic current of the baryons with a spin of 1/2 characterize two independent scalar func- tions F1(q2) and F2(q2) depending on q2, which are the Dirac and Pauli form factors, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' While the corresponding electrical and magnetic form factors GE(q2) and GM(q2) are written as [38, 46, 47], GE(q2) = F1(q2) + τF2(q2), (2) GM(q2) = F1(q2) + F2(q2), (3) where M is the baryon mass and τ = q2/(4M 2).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' With GE(q2) and GM(q2), the magnitude of the effective form fac- tor |Geff(q2)| is defined as |Geff(q2)| = � 2τ|GM(q2)|2 + |GE(q2)|2 1 + 2τ .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (4) In the time-like region, the effective form factors of hyper- ons are experimentally studied via the electron-positron anni- hilation processes.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Under the one photon exchange approx- imation, the total cross section of the annihilation reaction e+e− → ¯Y Y can be expressed in terms of the effective form factor Geff as [44, 48, 49] σe+e−→ ¯Y Y = 4πα2βCY 3s (1 + 1 2τ ) | Geff(s) |2, (5) with α = e2/(4π) = 1/137.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='036 the fine-structure con- stant, and β = � 1 − 4M 2 Y /s is a phase-space factor.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Here, s = q2 is the invariant mass square of the e+e− system.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The coulomb enhancement factor CY accounts for the electromag- netic interaction of charged point-like fermion pairs in the fi- nal state [50], which is given by CY = � y 1−e−y for Σ+, Σ−, and Ξ−, 1 for Σ0 and Ξ0, (6) with y = απ β 2MY √s .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Considering the CY factor, it is expected that the cross section of process e+e− → Y ¯Y is nonzero at the reaction threshold for charged hyperons pairs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' As plotted in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 1 for the case of Ξ− 1, the factor CY affects only at the energy region very close to the reaction threshold, and it decreases very quickly as the reaction energy growing and it follows that few MeV above the reaction threshold it is CY ∼ 1, then its effect can be neglected [50–53].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The EMFFs of Σ hyperon In the VMD model, the virtual photon couples to Σ and ¯Σ through isovector ρ0 meson and isoscalar ω and φ mesons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Since both the ω and φ are far from the mass threshold of Σ¯Σ, the behavior of the contributions from them are similar, thus we combine their contributions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In this way, one can param- eterize Dirac and Pauli form factors for Σ+ and Σ− in the 1 The numerical results for Σ+ and Σ− are similar.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 3 0 1 2 3 4 5 6 7 8 9 10 √ s − 2M Ξ − (MeV) 0 2 4 6 8 10 12 C Ξ − FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 1: The Coulomb factor for Ξ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' time-like region as follows [17,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 19],' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 2 F Σ+ 1 = g(q2)(f Σ+ 1 + βρ √ 2Bρ − βωφ √ 3 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (8) F Σ+ 2 = g(q2)(f Σ+ 2 Bρ − αωφ √ 3 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (9) F Σ− 1 = g(q2)(f Σ− 1 − βρ √ 2Bρ − βωφ √ 3 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (10) F Σ− 2 = g(q2)(f Σ− 2 Bρ − αωφ √ 3 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (11) F Σ0 1 = g(q2)(βωφ √ 3 − βωφ √ 3 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (12) F Σ0 2 = g(q2)µΣ0Bωφ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (13) with Bρ = m2 ρ m2ρ − q2 − imρΓρ ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (14) Bωφ = m2 ωφ m2 ωφ − q2 − imωφΓωφ ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (15) where the widths of ρ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' ω and φ are taken into account.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In this work, we take mρ = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='775 MeV, Γρ = 149.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1 MeV, Γωφ = 2 We have followed: |Σ+ ¯Σ−⟩ = 1 √ 2 |1, 0⟩ + 1 √ 3 |0, 0⟩ + 1 √ 6 |2, 0⟩ , |Σ− ¯Σ+⟩ = − 1 √ 2 |1, 0⟩ + 1 √ 3 |0, 0⟩ + 1 √ 6 |2, 0⟩ , |Σ0 ¯Σ0⟩ = − 1 √ 3 |0, 0⟩ + � 2 3 |2, 0⟩ , (7) with the basis of |IΣ¯Σ, IZ Σ¯Σ⟩.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In the one photon exchange approximation, there is no contributions from the isospin tensor terms.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (Γω + Γφ)/2 = 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4645 MeV, and mωφ = (mω + mφ)/2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9005 GeV, which are quoted in the review of particle physics book [54].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Besides, we take µΣ+ = 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='112ˆµΣ+, µΣ− = −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='479ˆµΣ−, µΣ0 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='044ˆµΣ0 in natural unit [54], i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=', ˆµ = e 2MΣ .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In addition, at q2 = 0, with the constraints GΣ+ E = 1 and GΣ+ M = µΣ+, GΣ− E = −1 and GΣ− M = µΣ−, the coefficients f Σ+ 1 and f Σ+ 2 , f Σ− 1 and f Σ− 2 can be calculated, f Σ+ 1 = 1 − βρ √ 2 + βωφ √ 3 , f Σ+ 2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='112 + αωφ √ 3 , (16) f Σ− 1 = −1 + βρ √ 2 + βωφ √ 3 , f Σ− 2 = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='479 + αωφ √ 3 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (17) Finally, the model parameters γ, the coefficients βρ, βωφ, and αωφ will be determined by fitting them to the experimental data on the time-like effective form factors of Σ+, Σ0, and Σ−, which will be discussed in following.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The EMFFs of Ξ hyperon For the case of e+e− → Ξ−¯Ξ+ and Ξ0¯Ξ0 reactions, since Ξ− and Ξ0 are isospin doublets, we express the Ξ−¯Ξ+ and Ξ0¯Ξ0 states in terms of isospin 0 and 1 components.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The mix- tures of isoscalar and isovector for Ξ−¯Ξ+ and Ξ0¯Ξ0 of equal relative wight but different sign are imposed by the isospin symmetry as introduced by the underlying Clebsch-Gorden coefficients [54].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Then,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' the Dirac and Pauli form factors F1 and F2 for Ξ− and Ξ0 can be easily obtained as before for the Σ hyperon,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' F Ξ− 1 = g(q2)(f Ξ− 1 − βρ √ 2 Bρ − βV1 √ 2 BV1 −βV2 √ 2 BV2 + βωφ √ 2 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (18) F Ξ− 2 = g(q2)(f Ξ− 2 Bρ − αV1 √ 2 BV1 −αV2 √ 2 BV2 + αωφ √ 2 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (19) F Ξ0 1 = g(q2)(f Ξ0 1 + βρ √ 2 Bρ + βV1 √ 2 BV1 +βV2 √ 2 BV2 + βωφ √ 2 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (20) F Ξ0 2 = g(q2)(f Ξ0 2 Bρ + αV1 √ 2 BV1 +αV2 √ 2 BV2 + αωφ √ 2 Bωφ),' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (21) with BV 1 = M 2 V1 M 2 V1 − q2 − iMV1ΓV1 ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (22) BV 2 = M 2 V2 M 2 V2 − q2 − iMV2ΓV2 ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (23) where we have considered contributions from two more ex- cited vector mesons,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' V1 and V2,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' in addition the contribu- tions from ground states ρ,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' ω and φ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Their mass and width 4 are MV1 (MV2) and ΓV1 (ΓV2), respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The mass MV2 and width ΓV2 are taken as used in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [7], which are: MV2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='993 GeV and ΓV2 = 88 MeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Besides, we take µΞ− = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='915ˆµΞ−, and µΞ0 = −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='749ˆµΞ0 in natural unit [54].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Then the coefficients f Ξ− 1 , f Ξ− 2 , f Ξ0 1 , and f Ξ0 2 can be calculated as f Ξ− 1 = −1 + βρ √ 2 + βV1 √ 2 + βV2 √ 2 − βωφ √ 2 , (24) f Ξ− 2 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='085 + αV1 √ 2 + αV2 √ 2 − αωφ √ 2 , (25) f Ξ0 1 = − βρ √ 2 − βV1 √ 2 − βV2 √ 2 − βωφ √ 2 , (26) f Ξ0 2 = −1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='749 − αV1 √ 2 − αV2 √ 2 − αωφ √ 2 .' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' (27) The parameter γ will be fixed as the one determined from the case of Σ, while the other free parameters βωφ, βρ, βV1, βV2, αωφ, αV1, αV2, ΓV1, and MV1 are determined by fitting them to experimental data on the time-like effective form factors of Ξ− and Ξ0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' III.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' NUMERICAL RESULTS Under the above formulations, we perform a four-parameter (γ, βρ, βωφ, αωφ)-χ2 fit to the experimental data on the ef- fective form factors Geff of Σ+, Σ0, and Σ− hyperons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' There are 33 data points in total, which are extracted at the center- of-mass energies from 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3864 to 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0200 GeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The fitted pa- rameters are: γ = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='527 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='024 GeV−2, βρ = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='63 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='07, βωφ = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='08 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='06, and αωφ = −3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='18 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='77.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' And the obtained χ2/dof is 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='69, where dof is the number of dimen- sion of the freedom.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Note that the obtained χ2/dof is larger than 1, since we have fitted all the experimental data from BESIII [9, 10], Belle [12], and BABAR [45] Collaborations, by considering these contributions from only ground state of vector mesons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' If we considered only these data of BESIII Collaboration [9, 10], the obtained χ2/dof is 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='17.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 2 we show the theoretical results of the effective form factors of the Σ+, Σ0, and Σ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The red, blue, and green curves stand for the results for Σ+, Σ0, and Σ−, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The exper- imental data from BESIII [9, 10], Belle [12], and BABAR Collaboration [45] are also shown for comparing.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' One can see that, with same model parameters, we can describe these data on the effective form factors of Σ+, Σ0 and Σ− quite well, especially for the precise data measured by the BESIII Collaboration [9, 10].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The total cross sections of e+e− → Σ¯Σ are also calculated with these fitted parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The numeri- cal results are shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 3, compared with the experimen- tal data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Since the effective form factors of Σ hyperons can be well reproduced with our model, the total cross sections of e+e− → Σ+ ¯Σ−, e+e− → Σ0 ¯Σ0 and e+e− → Σ− ¯Σ+ reactions can be also well described.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' For the case of Ξ− and Ξ0 effective form factors, γ is taken as the result of fitting to Σ hyperon, i.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='e.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=', γ = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='527, we per- form nine-parameter (βωφ, βρ, βV1, βV2, αωφ, αV1, αV2, ΓV1, MV1)-χ2 fit to the experimental data on.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' There are totally 18 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1 √ s (GeV� 10 −3 10 −2 10 −1 10 0 10 1 |Geff| Σ + BESIII Σ 0 BESIII Σ − BESIII Σ + Belle Σ 0 Belle Σ 0 BABAR FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 2: The obtained effective form factors of Σ+, Σ0, and Σ−, compared with the experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1 √ s (GeV� 10 −1 10 0 10 1 10 2 10 3 10 4 σ(pb) Σ + BESIII Σ 0 BESIII Σ − BESIII Σ + Belle Σ 0 Belle Σ 0 BABAR FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 3: The total cross section of Σ+, Σ0 and Σ− hyperons com- pared with experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' data points, and these data correspond to the center-of-mass energies from 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='644 to 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='080 GeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The fitted parameters are listed in Table II, with a reasonably small χ2/dof = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='29.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Since we have more free parameters and the experimental data points is limited, we did not get the uncertainties of these pa- rameters from the χ2 fit.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 4, we depict the effective form factor of the Ξ− and Ξ0 using the fitted parameters shown in Table II.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The red curve stands for the results of Ξ0, while the green curve is the fitted results for Ξ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Again, one can see that the experimental data on the effective form factors of Ξ− and Ξ0 can be well reproduced.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It is worth to mention that the two resonances V1 and V2 are crucial to describe the experimental data, and without their contributions, we cannot get a good fit to the experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In addition, the total cross section of e+e− → Ξ−¯Ξ+ and e+e− → Ξ0¯Ξ0 are also calculated with 5 TABLE II: Fitted model parameters for the effective form factors of Ξ− and Ξ0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Parameter Value Parameter Value βωφ −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='774 αωφ 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='346 βρ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='616 αV1 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='039 βV1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='099 αV2 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='113 βV2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='115 ΓV1 (MeV) 71 MV1 (GeV) 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='742 the fitted parameters shown in Table II, and the numerical re- sults are shown Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The two peaks of V1 and V2 can be clear seen, and more precise data around 2744 and 2993 MeV are needed to further study their properties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' We next pay 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1 √ s (GeV� 10 −2 10 −1 10 0 |Geff| Ξ − BESIII Ξ 0 BESIII FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 4: The obtained effective form factors of Ξ− and Ξ0 compared with the experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' attention to the EMFFs at the space-like region, which can be straightforwardly obtained with the these parameters de- termined from the experimental data in the time-like region.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Since the EMFFs in the space-like region are real, thus we have to ignore the widths of the vector mesons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Then one can calculate the mean squared charge radius, which is defined by the relation [1, 40, 55] � r2 ch � = \uf8f1 \uf8f4 \uf8f4 \uf8f2 \uf8f4 \uf8f4 \uf8f3 −6 GE(0) dGE(Q2) dQ2 ���� Q2=0 , for Σ+, Σ− and Ξ−, −6 dGE(Q2) dQ2 ���� Q2=0 , for Σ0 and Ξ0, (28) with Q2 = −q2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' With the parameters fitted above, the cal- culated results of � r2 ch � of Σ and Ξ hyperons are shown in Table III.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Our result for Σ− is agreement with the experi- mental data within uncertainties: � r2 ch � Σ− = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='61 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='12 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='09 [1], � r2 ch � Σ− = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='91 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='32 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4 [2].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [1] the Σ− charge radius was measured in the space-like Q2 range 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='035 − 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='105 GeV2 by elastic scattering of a Σ− beam off atomic electrons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The measurement was performed with the SELEX (E781) spectrometer using the Fermilab hyperon 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='6 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='8 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1 √ s (GeV� 10 −1 10 0 10 1 10 2 10 3 σ(pb) Ξ − BESIII Ξ 0 BESIII FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 5: The total cross sections of e+e− → Ξ−¯Ξ+ and e+e− → Ξ0¯Ξ0 reactions compared with experimental data.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' beam at a mean energy of 610GeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [2] it was at- tracted from the elastic scattering of high energy Σ− off elec- trons from carbon and copper targets using the CERN hy- peron beam, where these events are identified using a maxi- mum likelihood technique exploring the kinematical relations of the scattered particles.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Theoretical calculations with chi- ral perturbation theory (ChPT) [40, 56] and the nonlocal chi- ral effective theory (ChET) [57], and chiral constituent quark model (ChCQM) [58] are also listed for comparison.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' On can see that the orderings of the most charge radii calculated by other works are in agreement with our results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Moreover, our results are consistent with these calculations in Refs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [56–58] that � r2 ch � Σ+ > � r2 ch � Σ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' On the contrary, the results ob- tained with chiral perturbation theory predictions in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [40] indicate that the charge radius of Σ− is larger than the one of Σ+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In addition, the charge radius of Ξ0 calculated here is small and negative, which is in agreement with the nonlocal chiral effective theory calculation in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [57].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It is expected that these results can be tested by future experimental mea- surements.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' IV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' SUMMARY In this work, we study the effective form factor of Σ and Ξ hyperons in time-like region within the vector meson dom- inance model, and we take a common model parameter γ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' In addition, the effect of the isospin combination is taken into account.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' For the case of Σ hyperon, the contributions from ρ, ω and φ mesons are considered.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Within same model parame- ters, we can simultaneously describe the current experimental data on the effective form factors of Σ+, Σ0 and Σ−.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' While for the case of Ξ+ and Ξ−, in addition to the contributions of the ground states ρ, ω and φ, it is found that one needs also contributions from two new vector states, and their masses and widths are: MV1 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='742 GeV, ΓV1 = 71 MeV, MV2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='993 6 TABLE III: The obtained results for mean squared electromagnetic radii � r2 ch � (fm2) for Σ and Ξ.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' The results from two ChPT calculations, ChET and, ChCQM as well as the experimental data are also listed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Baryon Ξ0 Ξ− Σ+ Σ0 Σ− This work −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='07 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='43 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='78 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='12 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='65 ChPT [40] 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='13 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='03 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='49 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='05 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='60 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='03 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='67 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='03 ChPT [56] 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='36 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='61 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='99 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='03 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='780 ChET [57] −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='015 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='007 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='601 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='127 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='719 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='116 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='010 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='004 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='700 ± 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='124 ChCQM [58] 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='091 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='587 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='825 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='089 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='643 GeV, and ΓV2 = 88 MeV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It is expected that new precise ex- perimental data at BESIII [59] can be used to further study their properties.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Finally, we would like to stress that thanks to the effects of the isospin combinations, the effective form factors of Σ+, Σ0 and Σ− can be simultaneously reproduced within the same model parameters by using the vector meson dominance model.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Again, the theoretical results obtained here also indicate that the vecor meson dominance model is a valid tool for studying the baryonic electromagnetic form factors at the time-like region.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' More precise data on the e+e− → Y ¯Y reactions can be used to improve our knowledge of hyperon effective form factors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Acknowledgements We warmly thank Profs.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xiong-Fei Wang and Xiao-Rong Zhou for useful comments and discussions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' This work is partly supported by the National Natural Science Founda- tion of China under Grant Nos.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 12075288, 11735003, and 11961141012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' It is also supported by the Youth Innovation Promotion Association CAS.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [1] I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Gough Eschrich et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [SELEX], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 522, 233-239 (2001) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/S0370-2693(01)01285-0 [arXiv:hep-ex/0106053 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [2] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Adamovich et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [WA89], Eur.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 8, 59-66 (1999) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1007/s100520050444 [3] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Jones et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [Jefferson Lab Hall A], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 84, 1398-1402 (2000) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='84.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1398 [arXiv:nucl-ex/9910005 [nucl-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [4] O.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Gayou et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [Jefferson Lab Hall A], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 88, 092301 (2002) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='88.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='092301 [arXiv:nucl-ex/0111010 [nucl-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [5] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 97, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3, 032013 (2018) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='97.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='032013 [arXiv:1709.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10236 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [6] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 124, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3, 032002 (2020) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='124.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='032002 [arXiv:1910.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='04921 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [7] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 103, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 012005 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='012005 [arXiv:2010.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='08320 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [8] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 820, 136557 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2021.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='136557 [arXiv:2105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='14657 [hep- ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [9] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 814, 136110 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2021.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='136110 [arXiv:2009.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01404 [hep- ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [10] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 831, 137187 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2022.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='137187 [arXiv:2110.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='04510 [hep- ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [11] X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wang and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Huang, Symmetry 14, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 65 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3390/sym14010065 [12] [Belle], [arXiv:2210.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='16761 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [13] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Belushkin, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Hammer and U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meissner, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 75, 035202 (2007) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='75.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='035202 [arXiv:hep-ph/0608337 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [14] E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Kuraev, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi-Gustafsson and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dbeyssi, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 712, 240-244 (2012) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='04.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='073 [arXiv:1106.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1670 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [15] I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lorenz, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Hammer and U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meißner, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 92, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3, 034018 (2015) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='92.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='034018 [arXiv:1506.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02282 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [16] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Mangoni, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Pacetti and E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi-Gustafsson, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 104, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='11, 116016 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='104.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='116016 [arXiv:2109.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='03759 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [17] F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Iachello, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Jackson and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lande, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 43, 191- 196 (1973) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/0370-2693(73)90266-9 [18] F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Iachello and Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wan, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 69, 055204 (2004) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='69.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='055204 [19] R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Bijker and F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Iachello, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 69, 068201 (2004) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='69.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='068201 [arXiv:nucl-th/0405028 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [20] Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Yang, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chen and Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lu, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 100, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7, 073007 (2019) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='073007 [arXiv:1902.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01242 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [21] Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Li, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dai and J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xie, Chin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 39, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 011201 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1088/0256-307X/39/1/011201 [arXiv:2107.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10499 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [22] J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Haidenbauer, U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meißner and L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dai, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 103, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 014028 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='014028 [arXiv:2011.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='06857 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [23] E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi-Gustafsson and M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rekalo, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 504, 291- 295 (2001) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/S0370-2693(01)00312-4 [24] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Bianconi and E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi-Gustafsson, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 114, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='23, 232301 (2015) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='114.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='232301 [arXiv:1503.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02140 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [25] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Bianconi and E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi-Gustafsson, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 93, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3, 035201 (2016) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='93.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='035201 [arXiv:1510.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='06338 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [26] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Nature Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 17, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='11, 1200-1204 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1038/s41567-021-01345-6 [arXiv:2103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='12486 7 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [27] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dai, Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Li, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Chang and J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xie, Chin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 46, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7, 073104 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1088/1674-1137/ac5f9c [arXiv:2112.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='06264 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [28] Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Yang, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dai, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Guo, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Haidenbauer, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Kang and U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meißner, [arXiv:2206.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01494 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [29] X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Cao, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dai and H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lenske, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 105, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='7, L071503 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='105.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='L071503 [arXiv:2109.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='15132 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [30] G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lepage and S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Brodsky, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 43, 545- 549 (1979) [erratum: Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 43, 1625-1626 (1979)] doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='43.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='545 [31] G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lepage and S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Brodsky, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 22, 2157 (1980) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='22.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2157 [32] Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Li and J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xie, Commun.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Theor.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 73, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='5, 055201 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1088/1572-9494/abea0f [arXiv:2012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02379 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [33] C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Perdrisat, V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Punjabi and M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Vander- haeghen, Prog.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Part.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 59, 694-764 (2007) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ppnp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2007.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='05.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='001 [arXiv:hep-ph/0612014 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [34] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Denig and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Salme, Prog.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Part.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 68, 113- 157 (2013) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='ppnp.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2012.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='09.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='005 [arXiv:1210.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4689 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [35] S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Pacetti, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Baldini Ferroli and E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomasi- Gustafsson, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rept.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 550-551, 1-103 (2015) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physrep.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2014.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='09.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='005 [36] V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Punjabi, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Perdrisat, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Jones, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Brash and C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Carlson, Eur.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A 51, 79 (2015) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1140/epja/i2015-15079-x [arXiv:1503.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='01452 [nucl-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [37] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Mangoni, SciPost Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Proc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 10, 021 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='21468/SciPostPhysProc.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='021 [arXiv:2110.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='12475 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [38] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Irshad, D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Liu, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zhou and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Huang, Symmetry 14, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 69 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3390/sym14010069 [39] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Anselmino, E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Predazzi, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ekelin, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Fredriksson and D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lichtenberg, Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Mod.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 65, 1199-1234 (1993) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/RevModPhys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='65.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1199 [40] B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Kubis and U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meissner, Eur.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 18, 747-756 (2001) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1007/s100520100570 [arXiv:hep-ph/0010283 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [41] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 124, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4, 042001 (2020) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevLett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='124.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='042001 [arXiv:1905.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='09001 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [42] L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xia, C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rosner, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wang, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zhou, F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Maas, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Fer- roli, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Hu and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Huang, Symmetry 14, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2, 231 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3390/sym14020231 [arXiv:2111.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='13009 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [43] X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zhou, L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Yan, R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ferroli and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Huang, Symmetry 14, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 144 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3390/sym14010144 [44] B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Aubert et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BaBar], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 73, 012005 (2006) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='73.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='012005 [arXiv:hep-ex/0512023 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [45] B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Aubert et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BaBar], Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 76, 092006 (2007) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='76.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='092006 [arXiv:0709.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1988 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [46] R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Sachs, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 126, 2256-2260 (1962) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='126.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2256 [47] J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Green, J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Negele, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Pochinsky, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Syrit- syn, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Engelhardt and S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Krieg, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 90, 074507 (2014) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='90.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='074507 [arXiv:1404.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4029 [hep-lat]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [48] S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Dobbs, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Tomaradze, T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Xiao, K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Seth and G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Bonvicini, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Lett.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B 739, 90-94 (2014) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='physletb.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2014.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='025 [arXiv:1410.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='8356 [hep- ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [49] J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Haidenbauer, X.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' W.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Kang and U.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meißner, Nucl.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A 929, 102-118 (2014) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1016/j.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='nuclphysa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='2014.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='06.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='007 [arXiv:1405.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1628 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [50] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Arbuzov and T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Kopylova, JHEP 04, 009 (2012) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1007/JHEP04(2012)009 [arXiv:1111.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4308 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [51] R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Baldini, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Pacetti, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zallo and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zichichi, Eur.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A 39, 315-321 (2009) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1140/epja/i2008-10716-1 [arXiv:0711.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1725 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [52] R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Baldini Ferroli, S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Pacetti and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zallo, Eur.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' A 48, 33 (2012) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1140/epja/i2012-12033-6 [arXiv:1008.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='0542 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [53] Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Cao, H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Qi, Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' F.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wang and H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Zheng, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 100, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='5, 054040 (2019) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='100.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='054040 [arXiv:1906.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='00356 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [54] R.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' L.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Workman et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [Particle Data Group], PTEP 2022, 083C01 (2022) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1093/ptep/ptac097 [55] H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Atac, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Constantinou, Z.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' E.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Meziani, M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Paolone and N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Sparveris, Nature Commun.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' 12, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1, 1759 (2021) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1038/s41467-021-22028-z [arXiv:2103.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='10840 [nucl- ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [56] A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Hiller Blin, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 96, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='9, 093008 (2017) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='96.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='093008 [arXiv:1707.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='02255 [hep- ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [57] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Yang and P.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wang, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' D 102, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='5, 056024 (2020) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevD.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='102.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='056024 [arXiv:2005.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='11971 [hep-ph]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [58] G.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Wagner, A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Buchmann and A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Faessler, Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Rev.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 58, 3666-3669 (1998) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1103/PhysRevC.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='58.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='3666 [arXiv:nucl-th/9809015 [nucl-th]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [59] M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Ablikim et al.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' [BESIII], Chin.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' Phys.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content=' C 44, no.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='4, 040001 (2020) doi:10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='1088/1674-1137/44/4/040001 [arXiv:1912.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'} +page_content='05983 [hep-ex]].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1dAzT4oBgHgl3EQfDfo-/content/2301.00976v1.pdf'}