|
|
|
|
LEADER |
01947 am a22002173u 4500 |
001 |
124809 |
042 |
|
|
|a dc
|
100 |
1 |
0 |
|a Kimchi, Itamar
|e author
|
100 |
1 |
0 |
|a Massachusetts Institute of Technology. Department of Physics
|e contributor
|
700 |
1 |
0 |
|a Sheckelton, John P.
|e author
|
700 |
1 |
0 |
|a McQueen, Tyrel M.
|e author
|
700 |
1 |
0 |
|a Lee, Patrick A.
|e author
|
245 |
0 |
0 |
|a Scaling and data collapse from local moments in frustrated disordered quantum spin systems
|
260 |
|
|
|b Springer Nature,
|c 2020-04-22T18:01:23Z.
|
856 |
|
|
|z Get fulltext
|u https://hdl.handle.net/1721.1/124809
|
520 |
|
|
|a Recently measurements on various spin-1/2 quantum magnets such as H3LiIr2O6, LiZn2Mo3O8, ZnCu3(OH)6Cl2 and 1T-TaS2-all described by magnetic frustration and quenched disorder but with no other common relation-nevertheless showed apparently universal scaling features at low temperature. In particular the heat capacity C[H, T] in temperature T and magnetic field H exhibits T/H data collapse reminiscent of scaling near a critical point. Here we propose a theory for this scaling collapse based on an emergent random-singlet regime extended to include spin-orbit coupling and antisymmetric Dzyaloshinskii-Moriya (DM) interactions. We derive the scaling C[H, T]/T ~ H−γFq[T/H] with Fq[x] = xq at small x, with q ∈ {0, 1, 2} an integer exponent whose value depends on spatial symmetries. The agreement with experiments indicates that a fraction of spins form random valence bonds and that these are surrounded by a quantum paramagnetic phase. We also discuss distinct scaling for magnetization with a q-dependent subdominant term enforced by Maxwell's relations. ©2018
|
520 |
|
|
|a U.S. Department of Energy, office of Basic Energy Sciences, Division of Materials Sciences and Engineering (grant no. DEFG02-08ER46544)
|
520 |
|
|
|a DOE (grant no. DE-FG02-03-ER46076)
|
655 |
7 |
|
|a Article
|
773 |
|
|
|t 10.1038/S41467-018-06800-2
|
773 |
|
|
|t Nature communications
|