Impurities in Frustrated Magnets Leon Balents, UCSB Disorder, Fluctuations, and Universality, 2008.
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Transcript of Impurities in Frustrated Magnets Leon Balents, UCSB Disorder, Fluctuations, and Universality, 2008.
Collaborators Doron Bergman (Yale) Jason Alicea (Caltech) Simon Trebst (MS Station Q) Lucile Savary (ENS Lyon)
What is frustration? Competing interactions
Can’t satisfy all interactions simultaneously
Optimization is “frustrating”
“People need trouble – a little frustration to sharpen the spirit on, toughen it. Artists do; I don't mean you need to live in a rat hole or gutter, but you have to learn fortitude, endurance. Only vegetables are happy.” – William Faulkner
Frustration: Constrained Degeneracy When kBT ¿ J, system (classically) is constrained
to ground state manifold Triangular lattice Ising antiferromagnet
One dissatisfied bond per triangle Entropy 0.34 kB / spin
Pyrochlore Heisenberg antiferromagnet
Pyrochlore “Spin ice”: 2 in/2 out Ising spins Pauling entropy ¼ ½ ln(3/2) kB / spin
Challenge: spin liquid regime Frustration leads to suppressed order
“Frustration parameter” f=CW/TN & 5-10 System fluctuates between competing ordered
states for TN<T<CW
What is the nature of the correlated liquid?
Spin liquid
Only one ¼ consistent with RVB/gauge theory!
Quantum Spin Liquids f = CW/TN =1 : quantum paramagnetism RVB and gauge theories…
Many recent experimental candidates Herbertsmithite kagome Na4Ir3O8 hyperkagome NiGa2S4 triangular s=1 -(BEDT) organic triangular lattice FeSc2S4 diamond lattice spin-orbital liquid
+ + …
One class: “dipolar” spin liquids Classical pyrochlore spin liquids are
“emergent diamagnets” Local constraint: Dipolar correlations
Youngblood and Axe, 1980Isakov, Moessner, Sondhi 2003
Y2Ru2O7: J. van Duijn et al, 2007
A Problem Signatures of spin liquid correlations in
neutron scattering are subtle Not peaks
Often single crystal neutron scattering in not available
Can impurities be clarifying? Impurities may induce observable distortions
in the correlated medium C.f. Friedel oscillation Long-range impurity interactions?
Can look for differences in impurity-induced glassy states Formation with even weak impurities? Unconventional properties and transitions?
Some experimental features Appearance of spin glass state for very
weak disorder (e.g. in kagome and spin ice materials)
Commonly observed T2 specific heat in glass state
NiGa2S4 – coherent spin waves in disordered state, without observable glass transition
MnSi – partial order: disordered spirals?
Strange spin glasses in HFMs SCGO: SrCr9pGa12-9pO19 s=3/2 kagome
• Tg independent of disorder at small dilution?• Unusual T2 specific heat?
• nearly H-independent!
Ramirez et al, 89-90.
Excitations from low T state“Early” dispersion relation
What is clear so far: Spin wave like modes at low T A “slow” low E mode throughout zone + A highly dispersive mode
C. Broholm
A-site spinel CoAl2O4
Structure factor consistent with frozen superposition of spirals
Unusual T2.5 heat
capacity
Back to the dipolar spin liquid… Ising Pyrochlore = dimer model
Down spin = dimer
Very generally, dimer models on bipartite lattices show dipolar phases at high temperature
T¿ J: 2 up and 2 down spins
2 “dimers” per diamond site
T¿ J: 3 up and 1 down spin
1 “dimer” per diamond siteIn a field
Dilution Replace magnetic atom by non-magnetic
one In dimer picture, this removes a link on
which a dimer may sit
+ -
2 un-satisfied tetrahedra Dipole source!
Indeed observe long-range disturbance
Random bonds Jij ! Jij+Jij
Degeneracy of different states obviously broken Expect: glassy state for kBT ¿ |Jij|
Q: What is the nature of the glass transition?
Numerical evidence of Saunders and Chalker for such behavior in classical Heisenberg pyrochlore (2007)
Expect unconventional transition General argument (Bergman et al, 2006):
Spin glass order parameter does not describe the dipolar correlations in the paramagnetic phase
Can be argued that transition should be described by a gauge theory in which the Higgs phenomena quenches the dipolar fluctuations in the low temperature state
Holds for any interactions (also non-random) that quench the entropy Recent examples studied by Alet et al and
Pickles et al
A simple and dramatic example Classical cubic dimer model
Hamiltonian
Model has unique ground state – no symmetry breaking.
Nevertheless there is a continuous phase transition! - Without constraint there is only a crossover.
Many open issues How do multiple non-magnetic impurities
interact in a dipolar spin liquid? What is the phase diagram of a bond-
diluted dimer model? Purely geometrical problem with no energy
scale! What is the nature of the glass transition
from a dipolar Ising spin liquid?
Other spin liquids? A-site spinels Many materials!
1 900
FeSc2S4
10 205
CoAl2O4
MnSc2S4
MnAl2O4
CoRh2O4 Co3O4
s = 5/2
s = 3/2
Frustration is due to competing exchange interactions on a diamond lattice Creates very large degeneracy but smaller than in pyrochlores
Ground state evolution Coplanar spirals
q0 12 JJ1/8
NeelEvolving “spiral surface”
85.012 JJ 2012 JJ4.012 JJ2.012 JJ
Spiral surfaces:
Monte Carlo: “order by disorder” Parallel Tempering Scheme
Tc rapidly diminishes
in Neel phase
“Order-by-disorder”,
with sharply reduced Tc
Reentrant Neel
“spiral spin liquid”
Effects of impurities? Competing tendencies
Break spiral degeneracy: stabilize order? Locally random: create glass?
What would Thomas do?
What would Thomas do? Use scaling
arguments!
Use scaling arguments!
Single impurity Q1: How does a single impurity affect the
spiral degeneracy? A1: far from the impurity, the system must
have a uniform spiral wavevector
A2: for given impurity, there is a finite energy, a(k), which depends upon the wavevector at infinity
A3: approach to the uniform state is power-law and anisotropic, but relatively fast
Divergent energy
Multiple impurities In general, several types of impurities may
be present In spinel, dominant impurity is “inversion”
defect – magnetic atom on B site. There are four such defects not equivalent by translations.
Each impurity has its own a(k) favoring different discrete k spiral states
J2/J1=0.2: (111) favored
Multiple Impurities Q2: Does a low but non-zero density of
impurities favor a disordered or ordered state?
A: ordered Because of stiffness energy (k)2 L,
wavevector tends to remain uniform over many impurities
Average energy favors discrete ordered states
J2/J1=0.2: <100> favored
Multiple Impurities Q2: Does a low but non-zero density of
impurities favor a disordered or ordered state?
A: ordered Because of stiffness energy (k)2 L, wavevector
tends to remain uniform over many impurities Average energy favors discrete
ordered states Fluctuations in impurity densities do not
destroy order, like weak random fields in 3d Ising model (Imry-Ma)
Na3Ir4O7 Hyperkagome A quantum paramagnet:
CW¼ -650K2500
2000
1500
1000
500
0
1 (
mol
Ir/
cm3 )
3002001000T (K)
Na4Ir3O8
H = 1 T
5d5 LS
Ir4+
S = 1/2
60
40
20
0Cm
/T (
mJ/
Km
ol I
r+T
i)
200150100500T (K)
8
6
4
2
0
S m (
J/K
mol
Ir+
Ti)
1.8
1.6
1.4
(1
0-3em
u/m
ol I
r)
1086420T (K)
2.0
1.8
1.6
1.4
10-3
x = 0
0.01 T0.1 T1 T5 T
Tg
1
0-3
em
u/m
ol Ir
» Const
C » T2
inconsistent with quasiparticle picture?
Same behavior in other s=1/2 materials!
0 10K
(P. Schiffer and I. Daruka PRB, 56, 13712(1997)
~ -4 K
6
4
2
0
C2
(10-2
emu/
Km
ol I
r)
0.40.30.20.10.0x (Ti)
0.16
0.12
0.08
0.04
0.00
nearly free spin/all spin
2500
2000
1500
1000
500
0
1 (
mol
Ir/
cm3 )
3002001000T (K)
Na4(Ir1 xTix)3O8
H = 1 Tx = 0
x = 0.05
x = 0.1x = 0.2
x = 0.3
Dilution (Ti doping) releases spins Two population fit of
Approximately 0.3B released per Ti!