2018
DOI: 10.1103/physrevb.97.184401
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Using first-principles calculations to screen for fragile magnetism: Case study of LaCrGe3 and LaCrSb3

Abstract: In this paper, we present a coupled experimental/theoretical investigation of pressure effect on the ferromagnetism of LaCrGe3 and LaCrSb3 compounds. The magnetic, electronic, elastic, and mechanical properties of LaCrGe3 and LaCrSb3 at ambient condition are studied by first-principles density-functional theory calculations. The pressure dependences of the magnetic properties of LaCrGe3 and LaCrSb3 are also investigated. The ferromagnetism in LaCrGe3 is rather fragile, with a ferro-to paramagnetic transition a… Show more

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Cited by 9 publications
(5 citation statements)
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“…The systems with the space group of P 6 3 / mmc , such as the Ising ferromagnet FeCr 2 Te 4 , the topological superconductor BaSn 3 , and the ferromagnetic nodal-line semimetal candidate Fe 3 GeTe 2 , have recently attracted essential interest, presumably due to the special crystalline symmetry, , which makes these systems promising topological nontrivial materials and worthy of both theoretical and experimental investigation. , Furthermore, the structure of NdCrGe 3 consists of chains of face-sharing Cr-centered octahedra, 1 ∞ [CrGe 6/2 ], aligned along the c axis, separated by Nd atoms. The chains expand infinitely along the c direction [Figure (a,b)], exhibiting 1D features. , The Nd atoms are coordinated by 12 Ge atoms in an anticuboctahedral geometry. , Owing to the 1D crystal structure and the P 6 3 / mmc space group, NdCrGe 3 should be a potentially fruitful system in further theoretical and experimental research. Previously, the single crystals of LnCrGe 3 (Ln = rear earths), which were as tiny as 0.5 mm, were fabricated, and the basic magnetic properties were measured but based on polycrystalline samples . We have investigated the critical behavior and magnetocaloric of PrCrGe 3 single crystal around the ferromagnetic transition…”
Section: Introductionmentioning
confidence: 99%
“…The systems with the space group of P 6 3 / mmc , such as the Ising ferromagnet FeCr 2 Te 4 , the topological superconductor BaSn 3 , and the ferromagnetic nodal-line semimetal candidate Fe 3 GeTe 2 , have recently attracted essential interest, presumably due to the special crystalline symmetry, , which makes these systems promising topological nontrivial materials and worthy of both theoretical and experimental investigation. , Furthermore, the structure of NdCrGe 3 consists of chains of face-sharing Cr-centered octahedra, 1 ∞ [CrGe 6/2 ], aligned along the c axis, separated by Nd atoms. The chains expand infinitely along the c direction [Figure (a,b)], exhibiting 1D features. , The Nd atoms are coordinated by 12 Ge atoms in an anticuboctahedral geometry. , Owing to the 1D crystal structure and the P 6 3 / mmc space group, NdCrGe 3 should be a potentially fruitful system in further theoretical and experimental research. Previously, the single crystals of LnCrGe 3 (Ln = rear earths), which were as tiny as 0.5 mm, were fabricated, and the basic magnetic properties were measured but based on polycrystalline samples . We have investigated the critical behavior and magnetocaloric of PrCrGe 3 single crystal around the ferromagnetic transition…”
Section: Introductionmentioning
confidence: 99%
“…3(b) and 4(b) was determined by the measurements with modified Bridgman pressure cells which may produce larger pressure gradients compared with piston-cylinder pressure cells. The ferromagnetic instability in LaCrGe 3 has been shown to be primarily driven by the Cr-Cr distance along the c axis [33], which would be the direction of higher pressure gradients in the previous measurements in Bridgman cells [24,32]. Therefore the results of the NMR measurements by utilizing the piston-cylinder pressure cells should be compared with the phase diagram of Fig.…”
Section: Resultsmentioning
confidence: 97%
“…Face-sharing octahedra of Ge atoms encompassing Cr in LaCrGe 3 imply that correlated 3 d -states not only hybridize to p -ones of surrounding ligands but also bond between each other 23 , justifying a general p - d orbital structure of the model (1). In turn, parametrization of the model can be extracted from the electronic properties of LaCrGe 3 ( i ) shallow d -level position 23,24 and 3 d nature of Cr valence states indicate U /| ε d | ≫ 1; ( ii ) general agreement with (La 3+ )(Cr 3+ )(Ge 2− ) 3 oxidation state 23 pinpoints n d < 1; ( iii ) bonding between 3 d -states twice smaller than their hybridization to p -states 23 suggests 2| t d | ≃ | V |.…”
Section: Resultsmentioning
confidence: 99%