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One-dimensional approach to frustrated magnets

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appendix algebraic correlations No local order parameter dimer LRO broken translational symmetry staggered magnetization gapless magnons, S=1 gapped magnons, ... – PowerPoint PPT presentation

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Title: One-dimensional approach to frustrated magnets


1
One-dimensional approach tofrustrated magnets
  • Akira Furusaki (RIKEN)
  • Collaborators Oleg Starykh (Utah)
  • Leon Balents (UCSB)

PRB 72, 094416 (2005)
2
Phases of antiferromagnets
  • Neel ordered phase
  • Valence Bond Solid
  • Spin liquid (RVB)
  • Tomonaga-Luttinger liquid (d1)

staggered magnetization
gapless magnons, S1
dimer LRO broken translational symmetry
gapped magnons, S1
No local order parameter
deconfined massive spinons, S1/2
algebraic correlations
deconfined massless spinons, S1/2
3
Frustrated antiferromagnets a route to exotic
spin liquids ?
(classical) antiferromagnets on frustrated
lattices have extensive ground-state degeneracy
Lifting degeneracy by quantum fluctuations
exotic phases ?
fractionalized spin liquids?
cf. fractional quantum Hall liquids Landau
levels with extensive degeneracy
interactions Laughlin states,
anyons,..
4
Geometric frustration
Lattices with triangles geometric
frustration
spins on a triangle interacting via
antiferromagnetic exchange
2d Triangular lattice -(ET)2X,
Cs2CuCl4. Kagome lattice 3d Pyrochlore
lattice spinel oxides,.
2-fold degeneracy
5
Pyrochlore most frustrated 3d lattice
Corner-sharing 3d lattice of tetrahedra (4 spins
in each)
On every tetrahedron
Extensive degeneracy tetrahedra
6
2-dimensional pyrochlore checkerboard lattice
corner-sharing geometry, but and are
not equivalent
S1/2 antiferromagnetic Heisenberg model
7
related 2d lattice models
  • J1-J2 model
  • Shastry-Sutherland model

J1 N.N. AF exchange J2 N.N.N. AF exchange
8
  • J1-J2 model

LRO
LRO
finite-temperature Ising transition
Maximal frustration
2d J1-J2 model
Anisotropic model
Starykh Balents, PRL (2004)
9
  • Shastry-Sutherland model Physica 108B, 1069
    (1981)

dimer
plaquette singlet
Neel
Koga and Kawakami, PRL 84, 4461 (2000)
10
Ground-state phase diagram ofthe checkerboard
model (2d pyrochlore)
earlier results
?
11
J1gtgtJ2
  • B. Canals PRB 65, 184408 (2002)
  • spin wave analysis J(q)

Eigenvector of lowest eigenstate
12
J1J2
  • Exact diagonalization Fouet et al., PRB 67,
    054411 (2003)
  • J1J2, up to N36 (N40)
  • ground state S0 2-fold degeneracy (Ngtgt1)

valence bond crystal (plaquette singlet)
many low-lying excited states in the S0 sector
13
  • Series expansion Brenig and Grzeschik, PRB 69,
    064420 (2004)

triplet dispersion
14
Quadrumer boson approximation
hard-core bosons
15
  • rewrite the Hamiltonian in terms of the T bosons
  • discard quartic and higher-order terms
  • quadratic approximation
  • diagonalization by Bogoliubov transformation
  • dispersion of triplet bosons

(1) unstable when
bosons condense at
Antiferromagnetic LRO Neel state
(2) unstable when
bosons condense at
Magnetic LRO
16
Comparison with 1/S
(a)
(b)
(c)
(d)
(e)
Tchernyshyov, Starykh, Abanov Moessner, PRB 68,
144422 (2003)
17
J1ltltJ2
decoupled spin chains
sliding Luttinger liquids ?
Starykh, Singh Levin, PRL 88, 167203 (2002)
AF coupling is frustrated.
18
A single Heisenberg chain (S1/2)
staggered dimerization
Low-energy theory
SU(2)1 WZW theory
19
Quasi LRO (algebraic correlations)
dominant correlations
staggered magnetization
Neel order
Dimer order (VBS)
staggered dimerization
uniform magnetization is subdominant
20
Weak perturbation J1
Inter-chain interaction
However, the and terms
are dangerously irrelevant!
21
2nd order perturbation in V
Operator Product Expansion
relevant operator allowed by symmetry
Mean-field analysis
crossed-dimer state
22
comparison with exact diagonalization (36 spins)
Sindzingre, Fouet, Lhuillier, PRB 66, 174424
(2002)
dimer-dimer correlations
23
Global phase diagram
  • scenario I direct transition between
    crossed-dimer and plaquette VBS

? 1st order transition or intermediate
coexistence phase
Continuous transitions are forbidden by
Landau-Ginzburg-Wilson theory.
24
  • scenario II crossed-dimer and plaquette VBS via
    an intermediate ordered phase

? 1st order transition or intermediate
coexistence phase
25
application to 3d pyrochlore
26
Summary
  • Global phase diagram of the AF Heisenberg model
    on the 2d-pyrochlore (checkerboard lattice)
  • 1d-approach can give some useful hints for
    understanding 2d and 3d frustrated magnets.

?
?
Neel
Plaquette
Crossed Dimer
PRB 72, 094416 (2005)
27
appendix
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