Phase diagram of the antiferromagnetic J 1-J2 spin-1 pyrochlore Heisenberg model

被引:0
|
作者
Hagymasi, Imre [1 ,2 ,3 ]
Niggemann, Nils [1 ,2 ,4 ,5 ]
Reuther, Johannes [1 ,2 ]
机构
[1] Helmholtz Zentrum Berlin Mat & Energie, Hahn Meitner Pl 1, D-14109 Berlin, Germany
[2] Free Univ Berlin, Dahlem Ctr Complex Quantum Syst & Fachbereich Phys, Arnimallee 14, D-14195 Berlin, Germany
[3] Inst Solid State Phys & Opt, HUN REN Wigner Res Ctr Phys, POB 49, H-1525 Budapest, Hungary
[4] Indian Inst Technol Madras, Dept Phys, Chennai 600036, India
[5] Indian Inst Technol Madras, Quantum Ctr Diamond & Emerging Mat QuCenDiEM Grp, Chennai 600036, India
关键词
QUANTUM; LIQUID;
D O I
10.1103/PhysRevB.110.224416
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the phase diagram of the antiferromagnetic J 1-J2 Heisenberg model on the pyrochlore lattice with S = 1 spins at zero and finite temperatures. We use a combination of complementary state-of-the-art quantum many-body approaches such as density matrix renormalization group (DMRG), density-matrix purification, and pseudo-Majorana functional renormalization group (PMFRG). We present an efficient approach to preserve the applicability of the PMFRG for spin-1 systems at finite temperatures despite the inevitable presence of unphysical spin states. The good performance of our methods is first demonstrated for the nearest-neighbor pyrochlore Heisenberg model where the finite-temperature behavior of the specific heat and uniform susceptibility show excellent agreement within PMFRG and density-matrix purification. Including an antiferromagnetic second-neighbor coupling we find that the nonmagnetic ground-state phase of the nearest-neighbor model extents up to J 2 / J 1 0.02 within DMRG, beyond which magnetic k = 0 long-range order sets in. Our PMFRG calculations find the phase transition in a similar regime J 2 / J 1 0.035(8) which, together with the DMRG result, provides a strong argument for the existence of a small but finite nonmagnetic ground-state phase in the spin-1 pyrochlore Heisenberg model. We also discuss the origin of discrepancies between different versions of the functional renormalization group concerning the location of this phase transition.
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页数:12
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