diff --git "a/1tAzT4oBgHgl3EQfe_wu/content/tmp_files/load_file.txt" "b/1tAzT4oBgHgl3EQfe_wu/content/tmp_files/load_file.txt" new file mode 100644--- /dev/null +++ "b/1tAzT4oBgHgl3EQfe_wu/content/tmp_files/load_file.txt" @@ -0,0 +1,867 @@ +filepath=/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf,len=866 +page_content='arXiv:2301.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='01444v1 [cond-mat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='str-el] 4 Jan 2023 Magnetic properties of the layered heavy fermion antiferromagnet CePdGa6 H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Ye,1 T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Le,1 H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Su,1 Y.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' N.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Zhang,1 S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' S.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Luo,1 M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' J.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Gutmann,2 H.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Q.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Yuan,1, 3, 4, 5 and M.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Smidman1,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' ∗ 1Center for Correlated Matter and Department of Physics,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Zhejiang University,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Hangzhou 310058,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' China 2ISIS Facility,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Rutherford Appleton Laboratory,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Chilton,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Didcot Oxon OX11 0QX,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' United Kingdom 3Zhejiang Province Key Laboratory of Quantum Technology and Device,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Department of Physics,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Zhejiang University,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Hangzhou 310058,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' China 4State Key Laboratory of Silicon Materials,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Zhejiang University,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Hangzhou 310058,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' China 5Collaborative Innovation Center of Advanced Microstructures,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Nanjing University,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Nanjing 210093,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' China (Dated: January 5,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 2023) We report the magnetic properties of the layered heavy fermion antiferromagnet CePdGa6,' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' and their evolution upon tuning with the application of magnetic field and pressure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CePdGa6 orders antiferromagnetically below TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K, where there is evidence for heavy fermion behavior from an enhanced Sommerfeld coefficient.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Our results are best explained by a magnetic ground state of fer- romagnetically coupled layers of Ce 4f-moments orientated along the c-axis, with antiferromagnetic coupling between layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At low temperatures we observe two metamagnetic transitions for fields applied along the c-axis corresponding to spin-flip transitions, where the lower transition is to a dif- ferent magnetic phase with a magnetization one-third of the saturated value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' From our analysis of the magnetic susceptibility, we propose a CEF level scheme which accounts for the Ising anisotropy at low temperatures, and we find that the evolution of the magnetic ground state can be explained considering both antiferromagnetic exchange between nearest neighbor and next nearest neighbor layers, indicating the influence of long-range interactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Meanwhile we find little change of TN upon applying hydrostatic pressures up to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 GPa, suggesting that significantly higher pressures are required to examine for possible quantum critical behaviors.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' I.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' INTRODUCTION Heavy fermion compounds are prototypical examples of strongly correlated electron systems, and have been found to host a range of emergent phenomena including unconventional superconductivity, complex magnetic or- der and strange metal behavior [1–3].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Ce-based heavy fermions contain a Kondo lattice of Ce-ions with an un- paired 4f electron, which can both couple to other 4f mo- ments via the Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction and undergo the Kondo interaction due to hybridization with the conduction electrons.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Here the RKKY interaction gives rise to long-range magnetic or- der, while the Kondo interaction favors a non-magnetic Fermi-liquid ground state with greatly enhanced quasi- particle masses.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Due to the small energy scales, the rel- ative strengths of these competing interactions can often be tuned by non-thermal parameters such as pressure, magnetic fields and chemical doping [4], and in many cases the magnetic ordering can be continuously sup- pressed to zero temperature at a quantum critical point (QCP).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' A major question for heavy fermion systems is the relationship between quantum criticality, and the dome of unconventional superconductivity sometimes found to encompass the QCP.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CeIn3 is a canonical example of this phenomenon, which at ambient pressure orders antiferro- magnetically below TN = 10.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 K, but exhibits a pressure- induced QCP around 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='6 GPa, which is surrounded by a superconducting dome with a maximum Tc of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K [5].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The layered CeMIn5 (M= transition metal) com- pounds consist of alternating layers of MIn2 and CeIn3 along the c-axis [6], and among the remarkable proper- ties is a significantly enhanced superconducting Tc for the M= Rh and Co systems, reaching over 2 K [7, 8], giving a strong indication that quasi-two-dimensionality is important for promoting heavy fermion superconduc- tivity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Meanwhile the Ce2MIn8 compounds correspond to a stacked arrangement of two units of CeIn3, and one of MIn2 [9], and are expected to have an intermediate degree of two dimensionality relative to CeMIn5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Cor- respondingly, the superconducting phases have lower Tc values of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 and 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='68 K for Ce2CoIn8 [10] and Ce2PdIn8 [11] at ambient pressure, and a maximum of Tc = 2 K at 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 GPa for Ce2RhIn8 [12].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand, these different series of related Ce-based heavy fermion sys- tems also exhibit different magnetic ground states and crystalline electric field (CEF) level schemes [13–17] and therefore it is challenging to disentangle the role of these factors from that of the reduced dimensionality.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The elucidation of the interplay between these different as- pects requires examining additional families of layered Ce-based heavy fermion systems for quantum critical be- haviors, as well as detailed characterizations of the mag- netic ground states and exchange interactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The properties of layered Ce-based heavy fermion gal- lides have been less studied than the indium-based sys- tems.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CeGa6 has a layered tetragonal structure (space group P4/nbm), with four Ga-layers between each Ce layer [18].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This compound orders magnetically below TN = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='7 K, and there is evidence for the build-up of magnetic correlations at significantly higher tempera- tures [19].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' A more layered structure is realized in the Ce2MGa12 (M= Cu, Ni, Rh, Pd, Ir, Pt) series, where the Ce-layers are alternately separated by four Ga-layers, and units of MGa6, leading to a larger interlayer separation 2 of the Ce-atoms [20, 21].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Several members of this series show evidence for both antiferromagnetism and heavy fermion behavior [20–25], where pressure can readily sup- press the antiferromagnetic transitions of Ce2NiGa12 and Ce2PdGa12 [26, 27], while evidence for field-induced crit- ical fluctuations is revealed in Ce2IrGa12 [25].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CePdGa6 has a different layered tetragonal structure (space group P4/mmm) displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 1(a), consist- ing of square layers of Ce-atoms, with each Ce con- tained in a CeGa4 prism, separated by PdGa2 layers [28].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Correspondingly, there is a distance between Ce- layers of 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='92 ˚A, while the nearest neighbor in-plane Ce- Ce separation is 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='34 ˚A, compared to respective values of 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='54 ˚A and 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='65 ˚A in CeRhIn5 [29].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CePdGa6 or- ders antiferromagnetically below TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K, and heavy fermion behavior is evidenced by an enhanced Sommer- feld coefficient [20, 28].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' As such, CePdGa6 is a good can- didate to look for novel behaviors arising in quasi-two- dimensional heavy fermion systems, but there is both a lack of detailed characterizations of the magnetic ground state, and no reports of the evolution under pressure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In addition, most measurements of CePdGa6 are reported in Ref.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 28, where the results are affected by the inclu- sion of an extrinsic antiferromagnetic phase Ce2PdGa12, which can be eliminated using a modified crystal growth procedure [20].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In this article we report detailed measurements of the magnetic properties of single crystals of CePdGa6, in- cluding their evolution upon applying magnetic fields and hydrostatic pressure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' We find that CePdGa6 orders an- tiferromagnetically in zero-field, where the Ce-moments are orientated along the c-axis and align ferromagneti- cally within the ab-plane, but there is antiferromagnetic coupling between layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At low temperatures, two meta- magnetic transitions are observed for fields along the c- axis, the lower of which corresponds to a spin-flip transi- tion to a phase with magnetization one-third of the sat- urated value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' From our analysis of the magnetic suscep- tibility, we propose a CEF level scheme which can ex- plain the low temperature Ising anisotropy, and we find that from considering interactions between the nearest- neighbor and next nearest neighbor Ce-layers, the field evolution of the magnetic state can be well accounted for.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' II.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' EXPERIMENTAL DETAILS Single crystals of CePdGa6 were grown using a Ga self- flux method with a molar ratio of Ce:Pd:Ga of 1:1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5:15 [20].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Starting materials of Ce ingot (99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='9%), Pd pow- der (99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='99%) and Ga pieces (99.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='99%) were loaded into an alumina crucible which was sealed in an evacuated quartz tube.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The tube was heated to 1150 ◦C and held at this temperature for two hours, before being rapidly cooled to 500 ◦C at a rate of 150 K/h and then cooled more slowly to 400 C at 8 K/h.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' After being held at 400 ◦C for two weeks, the tube was removed from the furnace, and centrifuged to remove excess Ga.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The 2 0 1 FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) (a) Crystal structure of CePdGa6 where the red, blue and green atoms correspond to Ce, Pd and Ga, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' J0 represents magnetic exchange in- teractions between nearest neighbor Ce atoms within the ab- plane, J1 is between nearest neighboring layers and J2 is between next nearest layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' An image of a typical single crystal of CePdGa6 is also displayed, where each square in the background is 2 mm × 2 mm.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (b) X-ray diffraction pat- tern measured on a single crystal of CePdGa6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The red dashes correspond to the positions of the (00l) Bragg peaks, indicat- ing that the [001] direction is perpendicular to the large face of the plate-like samples.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' obtained crystals are plate-like with typical dimensions 2 × 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 × 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 mm3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Note that when slower cooling rates of 6 K/h or 4 K/h were used, the resulting crystals were significantly smaller.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Single crystals of the non-magnetic analog LaPdGa6 were also obtained using a similar pro- cedure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The composition was confirmed using a cold field emission scanning electron microscope (SEM) equipped with an energy dispersive x-ray spectrometer.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The phase of the crystals were checked using both a PANalytical X’Pert MRD powder diffractometer using Cu-Kα radi- ation, and a Rigaku-Oxford diffraction Xtalab synergy single crystal diffractometer equipped with a HyPix hy- brid pixel array detector using Mo-Kα radiation.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The ob- tained lattice parameters from the single crystal diffrac- tion data of a = 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3446(3) ˚A and c = 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='9173(10) ˚A are pg c3 0 100 200 300 2 3 4 5 4 8 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 ( cm) T (K) T N ~ 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K ( cm) T (K) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) Temperature dependence of the re- sistivity ρ(T ) of CePdGa6 between 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 and 300 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The inset displays the low temperature resistivity, where there is a sharp anomaly at the antiferromagnetic transition.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' in excellent agreement with previous reports [28].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Mea- surements of a crystal using the powder diffractometer are displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 1(b), where all the Bragg peaks are well-indexed by the (00l) reflections of CePdGa6, demon- strating that the c-axis is perpendicular to the large face of the crystals.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Resistivity and specific heat measure- ments were performed in applied fields up to 14 T using a Quantum Design Physical Property Measurement Sys- tem (PPMS-14) down to 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 K, and to 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 K using a 3He insert.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Resistivity measurements were performed after spot welding four Pt wires to the surface, with the exci- tation current in the ab-plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Magnetization measure- ments were performed in the range 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 - 300 K in applied fields up to 5 T using a Quantum Design Magnetic Prop- erty Measurement System (MPMS) SQUID magnetome- ter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Heat capacity measurements under pressure were carried out in a piston cylinder cell, using an ac calori- metric method.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' III.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' RESULTS A.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Antiferromagnetic transition and CEF excitations of CePdGa6 Figure 2 displays the temperature dependence of the resistivity ρ(T ) of CePdGa6 between 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 and 300 K, which has a residual resistivity ratio [RRR = ρ(300 K)/ρ(2 K)] = 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' A broad shoulder is ob- served at around 50 K, which likely arises due to both the Kondo effect, and as a consequence of CEF excita- tions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At higher temperatures, quasilinear behavior is observed, which could be due to electron-phonon cou- pling.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' As shown in the inset, there is an anomaly at around TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K, below which ρ(T ) decreases more rapidly with decreasing temperature, which corresponds C m /T (J mol 1 K 2 ) T (K) Rln2 S m (J mol 1 K 1 ) C m (J mol 1 K 1 ) T (K) (b) CePdGa 6 LaPdGa 6 C (J mol 1 K 1 ) T (K) (a) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) (a) Magnetic contribution to the spe- cific heat Cm at low temperatures, where the red solid line shows the results from fitting with Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The inset shows the total specific heat C of CePdGa6 and the non-magnetic analog LaPdGa6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (b) Temperature dependence of Cm/T and the magnetic entropy Sm of CePdGa6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The pink dotted line displays the low temperature contribution to the specific heat calculated from the CEF scheme deduced from the analysis of χ(T ).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' to the antiferromagnetic transition reported previously [20], while no signature of the spurious transition at higher temperatures is detected [28].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The total spe- cific heat of CePdGa6 and nonmagnetic isostructural LaPdGa6 are shown in the inset of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(a).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The tem- perature dependence of the magnetic contribution to the specific heat Cm was estimated by subtracting the data of LaPdGa6, which is shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(a), while the spe- cific heat coefficient Cm/T and the magnetic entropy Sm of CePdGa6 are displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' A pronounced λ-like anomaly is observed at TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K, as is typi- cal for a second-order magnetic phase transition.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' For T > TN, Cm/T increases with decreasing temperature, and extrapolates to a relatively large zero temperature value of 250 mJ/mol K2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' As discussed below, the analysis of the magnetic susceptibility χ(T ) suggests the presence of a low lying CEF level, which could contribute to Cm/T in this temperature range.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The dotted line in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(b) shows the calculated Cm/T for the CEF level scheme de- 8030412JS12 300 e0 0S0 04 0 10 20 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 0 150 300 0 200 400 (b) (emu/mol) T (K) H = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T H // c H // ab (a) H = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 T H // c H // ab 1/( ) (mol/emu) T (K) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 4.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) (a) Low temperature magnetic sus- ceptibility χ(T ) of CePdGa6, with an applied field of µ0H = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T both parallel to the c-axis and within the ab-plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (b) Temperature dependence of 1/(χ-χ0) up to 300 K for 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 T applied along the two field directions, where the dashed and solid lines show the results from fitting with the CEF model described in the text.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' scribed below, which has a sizeable value in the vicinity of the transition.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Subtracting the contribution from the CEF at TN yields an estimate of γ ∼ 121.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 mJ/mol K2 associated with the ground state doublet, and such an enhanced value could arise both due to heavy fermion behavior, as well as the presence of short range magnetic correlations, as inferred in CeRhIn5[30, 31].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The data below TN were analyzed using [32]: Cm = γT + c∆7/2 SW √ T exp �−∆SW T � × � 1 + 39T 20∆SW + 51 32 � T ∆SW �2� (1) where the first term corresponds to the electronic con- tribution and the second term arises due to antiferro- magnetic spin-waves.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Here the coefficient c is related to the spinwave stiffness D via c ∝ D−3, while ∆SW is the spin-wave gap.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The results from fitting the zero-field data are displayed in the main panel of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(a), where γ = 121.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 mJ/mol K2 was fixed, yielding ∆SW = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 K and c = 23 mJ/mol K2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The moderate value of ∆SW is smaller than TN, unlike the layered heavy fermions gallides Ce2PdGa12 and Ce2IrGa12 where ∆SW > TN [24, 25], likely reflecting the weaker magnetocrystalline anisotropy in CePdGa6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The temperature dependence of the magnetic entropy Sm of CePdGa6 is also displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3(b), obtained by integrating Cm/T , where Cm/T was linearly extrapolated below 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At TN, Sm reaches 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='76R ln 2, which together with the expected sizeable con- tribution from the excited CEF level discussed above, suggests a reduced entropy corresponding to the ground state doublet due to Kondo screening.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Figure 4(a) displays the temperature dependence of the magnetic susceptibility χ(T ) of CePdGa6 at low tem- peratures, with an applied field of µ0H = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T along the c-axis and within the ab-plane, which both exhibit an anomaly at TN.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At low temperatures, χ(T ) is sig- nificantly larger for fields along the c-axis than in the ab-plane, demonstrating that the c-axis is the easy-axis of magnetization.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At TN, there is a peak in χ(T ) for H ∥ c, while for H ∥ ab χ(T ) weakly increases below TN, indicating that this corresponds to an antiferromagnetic transition with moments ordered along the easy c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At higher temperatures, the data above 100 K can be analyzed using the Curie-Weiss law: χ=χ0+C/(T − θCW), where χ0 is a temperature-independent term, C is the Curie constant and θCW is the Curie-Weiss tem- perature, yielding θc CW = −11.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='7(3) K and an effective moment of µc eff = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='35µB/Ce for H ∥ c, as well as θab CW = −12.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='9(8) K and µab eff = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='49µB/Ce for H ∥ ab.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The obtained values of µeff for both directions are close to the full value of 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='54 µB for the J = 5 2 ground state multiplet of Ce3+.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At lower temperatures, there is a devi- ation of χ(T ) from Curie-Weiss behavior, due to the split- ting of the ground state multiplet by crystalline-electric fields.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' To analyze the CEF level scheme, we considered the following Hamiltonian for a Ce3+ ion in a tetragonal CEF [33] HCF = B0 2O0 2 + B0 4O0 4 + B4 4O4 4 (2) where Om l and Bm l are Stevens operator equivalents and parameters, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The B0 2 parameter can be es- timated from the high temperature susceptibility using [34] B0 2 = 10kB � θab CW − θc CW � 3(2J − 1)(2J + 3) , (3) where J = 5 2 for the ground state multiplet of Ce3+, yielding B0 2 = -0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='01077 meV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' χ(T ) along both directions was analyzed taking into account the contribution from the CEF χi CEF, as well as molecular field parameters λi using χi = χi 0 + χi CEF 1 − λiχi CEF , (4) where the superscript i denotes the c-axis or ab-plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' With B0 2 fixed from Eq.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 3, values of B0 4 = -0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0746 meV and |B4 4| = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='496 meV were obtained, together with molecular field parameters of λc = -3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='55 mol/emu and λab = 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='15 mol/emu, χc 0 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 × 10−4emu/mol and χab 0 = −2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 × 10−3emu/mol, and the fitted re- sults are shown in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 4(b).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' These parameters yield a CEF scheme with a Γ7 ground state Kramer’s doublet ��ψ± 1 � = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='883 ��± 5 2 � − 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='469 ��∓ 3 2 � (for positive B4 4), and excitations to Γ6 and Γ7 levels of ∆1 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 meV and ∆2 = 32.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 meV, respectively.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At high temperatures, the small 5 4 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 0 4 6 8 10 12 4 8 (b) (a) C P /T (J/mol K 2 ) T (K) 0 1 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 2 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 3 H // c 0 H (T) T (K) 0 H (T) H // ab FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) Temperature dependence of the spe- cific heat of CePdGa6 in various applied magnetic fields (a) parallel to the c-axis, and (b) within the ab-plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 4 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 4 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='04 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='06 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='08 4 8 (a) (emu/mol) T (K) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 1 H // c 0 H (T) 0 H (T) H // ab 1 2 4 6 8 (emu/mol) T (K) (c) (b) T (K) 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 2 3 H // c 0 H (T) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) Temperature dependence of the mag- netic susceptibility χ(T ) of CePdGa6 in different magnetic fields parallel to the c-axis for fields (a) below, and (b) above 1 T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The vertical arrows mark the position of the antiferro- magnetic transition.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Panel (c) shows χ(T ) for various fields applied within the ab-plane, where the dashed line shows the evolution of TN with field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' negative B0 2 leads to a nearly isotropic χ(T ), while at low temperatures, the negative B0 4 leads to the observed Ising anisotropy with an easy c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The predicted moment along the c-axis is given by ⟨µz⟩ = � ψ± 1 |gJJz| ψ± 1 � = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 µB/Ce, which is larger than the value obtained from the saturated magnetization.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The positive value of λab is consistent with ferromagnetic coupling between spins within the basal plane, while the smaller negative λc is consistent with weaker antiferromagnetic coupling be- tween Ce layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' B.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Field dependence of the magnetic properties In order to determine the behavior of the magnetic ground state in magnetic fields, and to map the field- temperature phase diagrams, measurements of the spe- H // ab H // c (b) H // c T (K) 2 3 4 M ( /Ce) 0 H (T) H // c (a) M ( /Ce) 0 H (T) M ( /Ce) 0 H (T) 5 K 3 K 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 K ( cm) 0 H (T) 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 K FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 7.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) (a) Isothermal field dependence of the magnetization M(H) of CePdGa6 for fields along the c-axis, at three temperatures below TN.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The lower inset displays the low field region of the data in the main panel, demonstrating hysteresis about the metamagnetic transition, while the up- per inset shows M(H) at 2 K for fields within the ab-plane.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (b) Field dependence of the resistivity ρ(H) of CePdGa6 at several temperatures for fields along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The dashed lines show the evolution of the two metamagnetic transitions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' cific heat and magnetization were performed in differ- ent applied fields.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Figure 5(a) displays the low tempera- ture specific heat of CePdGa6 with different fields applied along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' It can be seen that TN is gradually sup- pressed with increasing field, and at fields greater than 2 T, no magnetic transition is observed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Instead, there is a broad hump in C/T , which shifts to higher tempera- ture with increasing field, corresponding to the Schottky anomaly from the splitting of the ground state doublet in the applied field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 5(b), C/T is displayed for fields within the ab-plane, where the antiferromagnetic transition is more robust than for fields along the c-axis, and the broad Schottky anomaly is only clearly resolved in a field of 12 T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The differences in the field dependence for the two different field directions is consistent with the low temperature Ising anisotropy in CePdGa6, where a smaller field along the easy c-axis can bring the system to the spin-polarized state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The low temperature χ(T ) in different applied fields 744 00.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 己.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content="0 T0 0'288ST 088880." metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='00 V2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0--4806 2 4 6 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 C ac /T (a.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='u.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=') T (K) 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='20GPa 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='85GPa 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='60GPa 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='20GPa P (GPa) FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) Temperature dependence of the ac heat capacity of CePdGa6 at various hydrostatic pressures up to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 GPa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The vertical dashed line shows the position of the ambient pressure TN, which remains nearly unchanged with pressure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' are displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' For fields along the c-axis dis- tinctly different behaviors are observed for different field ranges.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In a field of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T, there is a sharp peak at TN, corresponding to entering the antiferromagnetic ground state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At a larger field of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 T, only a small hump is observed at TN, while at low temperatures there is an increase in χ(T ), and at higher fields there is broad peak which is gradually suppressed with field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Meanwhile for fields within the ab-plane up to at least 8 T, there is a gradual suppression of TN, in line with the specific heat results.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The isothermal magnetization as a function of field along the c-axis at three temperatures below TN is dis- played in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 7(a), measured upon both sweeping the field up and down.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In zero-field there is no remanent magnetization, consistent with a purely antiferromag- netic ground state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At 2 K, there are two metamagnetic transitions at Hm1 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 T and Hm2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T, where hysteresis is also observed indicating a first-order nature, whereas otherwise the magnetization plateaus, with only a weak change of the magnetization with field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This is consistent with Hm1 and Hm2 corresponding to spin-flip transitions, with the spins remaining orientated along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' For fields above Hm2, no magnetic transition is observed in the specific heat, and therefore this likely cor- responds to the system reaching the spin polarized state, with a saturation magnetization of Ms = 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 µB/Ce.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand, above Hm1 the magnetization reaches a value of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='35 µB/Ce, corresponding to ≈ Ms/3, in- dicating a change of magnetic structure with a ferro- magnetic component.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' While there is little change in the field-dependence of the magnetization at 3 K, the curves at 4 K are drastically different.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Instead of there being abrupt step-like metamagnetic transitions, the magneti- 0 1 2 3 4 0 2 4 6 0 1 2 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 H m2 H m1 H // c T (K) H (T) C (T) (T) (T) M (H) (H) M ( /Ce) 0 H (T) 2 K FIG.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 9.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' (Color online) Temperature-field phase diagram of CePdGa6 at ambient pressure for fields along the easy c-axis, from measurements of the resistivity, magnetization, and spe- cific heat.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The solid line shows the evolution of TN, while the dashed lines show the positions of the low temperature metamagnetic transitions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The magnetic structures at low temperature are also illustrated by the orange arrows, where in zero-field there is an antiferromagnetic ground state, while upon applying a field the system passes through an interme- diate ↑↑↓ phase, before entering the spin polarized state.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The inset shows the field dependence of the magnetization based on mean-field calculations of the magnetic ground state cal- culated using the McPhase software package [35], with the parameters described in the text.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' zation smoothly increases with field, reaching a very sim- ilar saturation value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This suggests that at higher tem- peratures, the spins continuously rotate upon increasing the applied field, rather than undergoing abrupt spin flip transitions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The field dependent magnetization at 2 K for fields in the ab-plane is also shown in the inset of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 7(a), which smoothly changes with field, with no sign of saturation up to at least 5 T, consistent with this being the hard direction of magnetization.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The metam- agnetic transitions are also revealed in the field depen- dence of the resistivity ρ(H), as displayed in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 7(b) for fields along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 K, two abrupt anomalies are observed corresponding to Hm1 and Hm2, which are also detected at 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8 K and 3 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Above these transitions, there is a decrease of ρ(H), consistent with the reduced spin-flip scattering arising from a larger ferromagnetic component to the magnetism.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand, no metamagnetic transitions are detected at 5 K, where in- stead there is a broad peak in ρ(H), again consistent with a more gradual reorientation of the spins with field at higher temperatures.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 7 C.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Magnetism of CePdGa6 under pressure To determine the evolution of the magnetic order un- der pressure, the temperature dependence of the ac spe- cific heat of CePdGa6 was measured at several differ- ent hydrostatic pressures up to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 GPa, which are dis- played in Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 8.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' It can be seen from the dotted line that there is little change of TN with pressure indicat- ing the robustness of magnetic order.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In the case of the layered Ce2MGa12 compounds, the TN of Ce2NiGa12 and Ce2PdGa12 decrease with pressure, and antiferro- magnetism is suppressed entirely above 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 and 7 GPa, respectively [26, 27].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand the TN of Ce2IrGa12 undergoes a moderate enhancement from 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 to 3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='7 K for pressures up to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3 GPa, indicating that this compound is located on the left side of the Doniach phase diagram [25].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In the case of CePdGa6, the robust- ness of TN suggests that measurements to higher pres- sures are required to situate this compound within the framework of the Doniach phase diagram and to exam- ine whether there is pressure-induced quantum criticality in CePdGa6.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' IV.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' DISCUSSION Our measurements of the resistivity, magnetic sus- ceptibility and specific heat show that CePdGa6 orders antiferromagnetically below TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K, with the mo- ments orientated along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Figure 9 displays the temperature-field phase diagram for magnetic fields ap- plied along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The phase boundaries obtained from different measurements are highly consistent, show- ing that TN shifts to lower temperatures with field, before abruptly disappearing in a field of 2 T.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' At low temper- atures, there are two step-like metamagnetic transitions shown by the dashed lines, where the second transition is to the spin polarized state, while the lower transition cor- responds to a change of magnetic state to a phase with a magnetization of 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='35 µB/Ce, about one-third of the saturated value.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Such step-like changes in the magne- tization suggest that the spins are strongly constrained along the c-axis, and therefore there are abrupt spin- flip transitions for fields applied along the ordering di- rection.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand, at 4 K the magnetization changes smoothly with field, reaching the same saturated magnetization, indicating that at this temperature the spins continuously rotate in the applied field.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Such a change with temperature may be a consequence of only a moderate magnetocrystalline anisotropy, as also evi- denced by the relatively small value of the spin-wave gap ∆SW /TN ≈ 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4, as compared to the other heavy fermion gallides Ce2IrGa12 and Ce2PdGa12 which have ∆SW /TN of 1.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='5 and 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='8, respectively [24, 25].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' From the analysis of the magnetic susceptibility includ- ing the CEF contribution, the molecular field parameter is positive in the ab-plane (λab), while a smaller negative value is obtained along the c-axis (λc).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Together with the fact that only a relatively small field along the c-axis is re- quired to reach the spin polarized state, this suggests that the antiferromagnetic ground state consists of ferromag- netically ordered Ce-layers coupled antiferromagnetically along the c-axis.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' The simplest model for such a system would consist of ferromagnetic Heisenberg exchange in- teractions between nearest neighbor Ce atoms within the ab-plane J0 > 0, and antiferromagnetic exchange inter- actions J1 < 0 between nearest neighboring layers, as well as a sufficiently strong Ising anisotropy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This yields an A-type antiferromagnetic ground state consisting of ferromagnetic layers with moments orientated along the c-axis, where the moment direction alternates between adjacent layers, “↑↓↑↓”.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This model however cannot ac- count for the field induced phase with one-third magneti- zation, since for fields along the c-axis, only a metamag- netic transition directly from the ↑↓↑↓ phase to the spin polarized state is anticipated.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In order to realize the intermediate field-induced phase, it is necessary to consider an antiferromagnetic exchange J2 between next nearest neighboring layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In this case, from considering the classical ground state energies with sufficiently strong Ising anisotropy, the same ↑↓↑↓ ground state is realized for J1/J2 > 2, while a ↑↑↓↓ state oc- curs for J1/J2 < 2 [36].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Upon applying a magnetic field along the c-axis, there is a metamagnetic transition at a field Hm1 to an ↑↑↓ state with a net magnetization one-third of the saturated value, and another at Hm2 to the spin polarized state, where Hm2/Hm1 is deter- mined by J1/J2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' We performed mean-field calculations of the magnetic ground state and magnetization using the McPhase software package [35], which determines the most stable magnetic structure at a given temper- ature and magnetic field from considering multiple ran- dom starting moment configurations.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' These took into account the Heisenberg exchange interactions described above, as well as the CEF Hamiltonian HCF with our de- duced values of the Stevens parameters.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' As shown in the inset of Fig.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' 9, the observed values of Hm1 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='4 T and Hm2 = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='1 T, from the midpoints of the metamagnetic transitions at 2 K, are well reproduced from the mean- field calculations at 2 K with J1 = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='023 meV and J2 = −0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='0085 meV, where for Hm1 < H < Hm2 the ↑↑↓ ground state has the lowest energy.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Keeping these values fixed, we find that a nearest neighbor in-plane ferromag- netic interaction J0 = 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='034 meV can yield the observed value of TN = 5.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 K.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Therefore our analysis suggests stronger in-plane ferromagnetic interactions, where the value of 4J0/(2J1 + 2J2) = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='16 is close to our fitted value of λab/λc = 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='3.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Note that here we have assumed a ↑↓↑↓ ground state with J1/J2 > 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Although a ↑↑↓↓ phase has been reported in CeCoGe3 [37], such a scenario is less likely in CePdGa6 due to the larger interlayer dis- tances.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Compared to the layered heavy fermion antiferromag- net CeRhIn5, the magnetism in CePdGa6 appears to have a much more three dimensional character, whereas it is rather two-dimensional in the former, with J1/J0 = 8 0.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='13 deduced from inelastic neutron scattering [38].' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In addition, in CeRhIn5 the easy plane anisotropy and pres- ence of in-plane antiferromagnetic interactions give rise to spiral magnetic order which is incommensurate along the c-axis [13, 14], and these features may be important factors for realizing the unconventional quantum critical- ity and superconductivity.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' On the other hand, the TN of CePdGa6 is much more robust with pressure, remaining almost unchanged at pressures up to 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 GPa.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Therefore an understanding of the relationship between the mag- netism and any quantum critical behaviors will require measurements at considerably higher pressures.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' In addition, despite the layered arrangement of Ce atoms, the local environment of the Ce atoms is rel- atively three dimensional, as evidenced by the derived CEF parameters being close to that for a cubic sys- tem (where B0 2 = 0 and |B4 4| = 5|B0 4|).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This CEF scheme can correctly predict the low-temperature Ising anisotropy, but the predicted moment along the c-axis is larger than that observed.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' While such a reduced mo- ment compared to that predicted from the CEF level- scheme is often observed in heavy fermion antiferromag- nets due to screening of the moments by the Kondo effect [14, 16, 37, 39, 40], confirming whether such a scenario is applicable to CePdGa6 requires a more precise determi- nation of the CEF parameters, by measurements such as inelastic neutron scattering.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' V.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' CONCLUSION In summary, we have characterized the magnetic prop- erties of the heavy fermion antiferromagnet CePdGa6, and their evolution upon the application of mag- netic fields and pressure.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' We have constructed the temperature-field phase diagram for fields along the c- axis, where at low temperatures there are two abrupt metamagnetic transitions corresponding to spin-flip tran- sitions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' From the analysis of the magnetic susceptibility, we propose a CEF level scheme for the splitting of the ground state J = 5/2 multiplet, indicating that the Ising anisotropy at low temperatures is driven by the sizeable B0 4 parameter.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Moreover, our results are consistent with an antiferromagnetic ground state consisting of ferromag- netically coupled Ce-layers, with antiferromagnetic cou- pling between layers.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' We have proposed a model for the exchange interactions which can explain the evolution of the magnetic ordering with applied magnetic field, which has sizeable nearest neighbor and next-nearest neighbor layer interactions, indicating the presence of significant long-range magnetic interactions.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' Despite evidence for heavy fermion behavior, there is negligible change of TN upon applying pressures up 2.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='2 GPa, and hence measure- ments at much higher pressures are necessary to look for evidence of quantum criticality.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' VI.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' ACKNOWLEDGMENTS We are grateful to Martin Rotter for advice with the McPhase software.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' This work was supported by the Na- tional Key R&D Program of China (2017YFA0303100), the Key R&D Program of Zhejiang Province, China (2021C01002), and the National Natural Science Foun- dation of China (12174332, 12034017 and 11974306).' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content=' ∗ msmidman@zju.' metadata={'source': '/home/zjlab/wf/langchain-ChatGLM/knowledge_base/1tAzT4oBgHgl3EQfe_wu/content/2301.01444v1.pdf'} +page_content='edu.' 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