probing continua of excitations in kitaev spin liquids
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Probing continua of excitations in Kitaev spin liquids
Natalia PerkinsUniversity of Minnesota
KITP, Intertwined17
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Collaborators
Brent Perreault (UMN)
Jeroen van den Brink(IFW, Dresden)
Gábor Halász (KITP,UCSB)
Fiona Burnell (UMN)
Gia-Wei Chern University of Virginia
Dima Kovrizhin Cambridge UK
Johannes Knolle Cambridge UK
Roderich Moessner MPIPKS, Dresden
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Quantum spin liquids
1973: Anderson proposes the “Resonating Valence Bond” state - a prototype of the modern QSLs
+ + … � =
QSL: State of interacting spins that breaks no rotational or translational symmetry and has only short range spin correlations.
QSLs are characterized by topological order and long range entanglement (difficult to probe experimentally).
QSLs supports excitations with fractional quantum numbers and statistics.
Unlike states with broken symmetry, QSLs are not characterized by any local order parameter.
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Example: Fractionalized excitations in spin-1/2 Heisenberg AFM chain
Mourigal et al, Nature Physics 2013
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Many different quantum spin liquids
• Topological gapped QSLs
Quantum dimer model, toric code model…
• Spinon Fermi surface QSLs
Triangular lattice quantum spin liquid (YbMgGaO4)
• Variety of Kitaev gapless QSLs with nodal Majorana fermion band structures
Hyperhoneycomb with nodal lines of Dirac cones, hyperoctagon with Majorana fermions Fermi surface..
• U(1) QSL with gapless emergent photon
Quantum spin ice
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Quantum spin liquids
Main Question:
How to probe QSLs and their statistics?
Take home message:
Signatures of quantum order are mainly in the excitations
excitation
Incident light, X-rays, neutrons … Scattered
light, X-rays, neutrons…
fractionalizedexcitations
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Since excitations carry fractional quantum numbers relative to the local degrees of freedom, only multiple quasiparticles can couple to external probes.
Response from QSL is always a multi-particle continuum
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Spinon excitations in spin-1/2 Heisenberg AFM chain
CuSO4·5D2O,
Mourigal et al, Nature Physics 2013
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KCuF3
Lake, Caux, Tennant 2013
Spinon excitations probed by neutrons:
The fractionalization was definitively identified by excellent quantitative agreement between experiments and exact calculation based on the Bethe Ansatz.
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Poor understanding of strongly interacting systems beyond 1D
Kitaev Spin Liquids
No exact results, only numerics or uncontrolled approximations
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Kitaev model on the honeycomb lattice
A. Kitaev, Annals of Physics 321, 2 (2006)
H = �X
x�bonds
Jx
�x
j
�x
k
�X
y�bonds
Jy
�y
j
�y
k
�X
z�bonds
Jz
�z
j
�z
k
Mapping spins to Majorana fermions:
Exactly solvable 2D model
Spin liquid ground state
Fractionalized excitation
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Spin fractionalization and Majorana fermions
Quadratic Hamiltonian in each flux sector:
Large number of conserved quantities, local plaquette operators:
uzij
ci
cj
The Hilbert space can be separated into sectors corresponding to eigenvalues
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Excitations in the 2D Kitaev spin liquid
Fig. from M. Hermanns et al, 2014
Flux excitations are always gapped.Majorana fermion (spinon) excitations are gapped or gapless.
Majorana fermion excitation spectrum in the gapless phase
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3D Kitaev family
H<0> H<1> H<1>
Hyperhoneycomb lattices
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3D Kitaev family
M. Hermanns et al, 2015
HyperoctagonHyperhexagon
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Experimental realizationsNa2IrO3
alpha-Li2IrO3
Y.Singh, P. Gegenwart, PRL 2010, 2011
K. Plumb et al, Phys. Rev. B (2014)A. Banerjee et al, Nature Materials (2016)
alpha-RuCl3
beta-Li2IrO3
T. Takayama et al, PRL (2015)
gamma-Li2IrO3
Modic,'Nature'Comminica1ons'5,'4203'(2014)'
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Hyperhoneycomb lattice
M. Hermanns et al, 2015
closed line of Dirac nodes
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Hyperoctagon latticeMajorana metal
Fermi surfaces
M. Hermanns et al, 2015
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Hyperhexagon lattice
gapless Weyl points
M. Hermanns et al, 2015
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Spectroscopy of Kitaev Spin Liquids
INS of Kitaev Spin Liquids (briefly)
Raman scattering in Kitaev Spin Liquids (briefly)
RIXS scattering in Kitaev Spin Liquids
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Inelastic neutron scattering of Kitaev Spin Liquids
Knolle, Kovrizhin, Chalker, Moessner, PRL (2014)
Measurement of a dynamic structurefactor S(q,𝜔) leads to a sudden insertion of a pair of Z2 gauge-fluxes
QSL: expected spin-excitation continuum vs sharp dispersive features for spin-waves
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Banerjee, et al., Nature Mat. (2016) Banerjee, et al., Science (2017)
RuCl3
Signatures of fractionalization are visible!
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Raman spectroscopy of Kitaev Spin Liquids
Photon-in photon-out process
Photon induced spin exchange
Devereaux, Hackl RMP 2007
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Raman Scattering in Kitaev model
Raman vertex: diagonal in fluxes but creates two Majorana fermions
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Raman Scattering results (2D)
isotropic point: polarization independent
Knolle, Chern, Kovrizhin, Moessner, NP (PRL 2014)
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Raman Scattering results (2D)
anisotropic point: polarization dependence
Knolle, Chern, Kovrizhin, Moessner, NP (PRL 2014)
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RuCl3
Big ‘hump’ with fine features of the Majorana DOS. Signatures of fractionalization are visible! (comparison gives JK~8meV)
L. Sandilands,Y.J. Kim, K.S. BurchPhys. Rev. Lett. 114 (2015)
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The Raman response is polarization dependent!
Brent Perreault, Johannes Knolle, NBP, F. J. Burnell, PRB 2015
Raman Scattering results (3D)
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Glamazda, Lemmens, Do, Choi, Choi, Nature Comm. 7 (2016)
𝛾-Li2IrO3
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RIXS spectroscopy of Kitaev Spin Liquids
L. J. P. Ament, M. van Veenendaal, T. P. Devereaux, J. P. Hill, J. van den Brink, RMP (2011)
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RIXS from Ir4+
(Na,Li)2IrO3 with Ir4+ in 5d 5 configuration [L3 edge]:
5d
2p
Core hole
Kitaev model: H = HK
Non-magnetic vacancy
Incoming photon: Q, ε
Outgoing photon: Q’, ε’
0 f
k,!k k0,!k0
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Halász, Chalker, Moessner, PRB 2014
1
23
4
56
XXX
The Kitaev model with a single vacancy at site r= the original Kitaev model with switched off couplings around site r (exactly solvable)
Description: the vacancy is always in the spin-up state and the couplings to NN are zero.
d†r,#| "i = | "i
d†r,#| #i = 0
d†r,"| "i = 0
d†r,"| #i = | "i
Intermediate state with a vacancy
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The four fundamental RIXS channels are introduced by decomposingthe polarization tensor into
(a) Spin-conserving (SC) channel with
RIXS amplitude for the Kitaev model
A↵�(m,q) =P
r,nr
hm|dr,↵|nrihnr|d†r,� |0i
⌦�En+i� eiq·r
I(!,q) =P
m |P
↵,� T↵�A↵�(m,q)|2 �(! � Em)
q ⌘ k� k0 Kramers−Heisenberg formula
(b) three non spin-conserving (NSC) channels with
and cyclic permutations
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The four fundamental RIXS channels
A(m,q) =X
⌫
P⌫A⌫(m,q)
A⌫(m,q) =X
r
eiqr e��t hm|�⌫r e
�itHr |0i
Spin-conserving (SC) channel:
A0(m,q) =X
r
eiqr e��t hm|e�itHr |0i
Az(m,q) =X
r
eiqr e��t hm|�zre
�itHr |0i
Three non spin-conserving (NSC) channels:
Ax(m,q) =X
r
eiqr e��t hm|�xr e
�itHr |0i
Ay(m,q) =X
r
eiqr e��t hm|�yr e
�itHr |0i
create two flux excitations
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Fast collision approximation
(Na,Li)2IrO3 and α-RuCl3 : Γ / Jx,y,z >> 1
t ~ 1 / Γ << 1 / Jx,y,z !
The lowest order RIXS amplitude is then
NSC channels recover INS amplitudes for infinite Γ
Flux creation: Finite gap, little dispersion
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Results: SC channel2D Kitaev model
Elastic response Inelastic response
xno flux and two fermion excitations
interference between the two sublattices
A B
|0i
I0(!,q) /Z
BZd2k �(! � "k � "q�k) ["k � "q�k]
2 ��1� ei'k ei'q�k��2
I0(!,q) =X
m
|A0(m,q)|2�(! � Em)
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RIXS response in SC channel
Reciprocal space
Γ
M K
K ~
M ~
BZ
EBZ
G. B. Halasz, NBP, J.van den Brink (PRL 2016)
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RIXS response in SC channel
Reciprocal space
Γ
M K
K ~
M ~
BZ
EBZ
Gapless response at a finite number of discrete points
Dirac points
K points
Gapless points
~ Γ, K, K points G. B. Halasz, NBP, J.van den Brink (PRL 2016)
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RIXS response in SC channel
Reciprocal space
Γ
M K
K ~
M ~
BZ
EBZ
20 ][),(~ kqkqk −−∝ εεI
the response actually vanishes at the and points due to the factor� K
G. B. Halasz, NBP, J.van den Brink (PRL 2016)
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RIXS response in SC channel
Reciprocal space
Γ
M K
K ~
M ~
BZ
EBZ
G. B. Halasz, NBP, J.van den Brink (PRL 2016)
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Results: SC channel in 3D Kitaev models
closed line of Dirac nodes Fermi surfacesgapless Weyl points
For each model, the low-energy(gapless) response is determined by the nodal structure of the fermions.
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Hyperhoneycomb lattice
The Majorana fermions are gapless along a nodal line within the Γ-X-Y plane.
The response is thus gapless in most of the Γ-X-Y plane and also in most ofthe Z-A-T plane. However, it is still gapped at a generic point of the BZ.
G. B. Halasz, B. Perreault, NBP (1705.05894)
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Hyperhexagon lattice
The fermions are gapless at Weyl points.
The response is thus only gapless at particular points of the BZ.
G. B. Halasz, B. Perreault, NBP (1705.05894)
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Hyperoctagon lattice
The Majorana fermions are gapless on a Fermi surface.
The response is thus gapless in most of the BZ.G. B. Halasz, B. Perreault, NBP (1705.05894)
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Thank you