Possible Kitaev spin liquid physics and topological ... · PowerPoint Presentation Author: Roy,...
Transcript of Possible Kitaev spin liquid physics and topological ... · PowerPoint Presentation Author: Roy,...
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Stephen Nagler
Oak Ridge National Laboratory
Possible Kitaev spin liquid physics and
topological transitions in a-RuCl3
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2 SEN CNLS 2019
Outline
I. Kitaev’s model• Quick reminder of possible relevance to materials
• Basics of a-RuCl3
II. Some inelastic neutron scattering• Magnons and fractional excitations in INS
• Inelastic neutron scattering in a-RuCl3
III. Recent results• Higher fields and 3rd dimension
• Magnetocaloric effect and T- B phase diagram
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3 SEN CNLS 2019
Neutron Scattering Collaborators:A. Banerjee, A. Aczel, C. Balz, C. Batista, S. Bhattacharjee, C.
Bridges, H. Cao, B. Chakoumakos, G. Ehlers, O. Garlea, G.
Granroth, Y. Kamiya, J. Knolle, D. Kovrizhin, P. Lampen-Kelley, L.
Li, Y. Liu, Z. Lu, M. Lumsden, D. Mandrus, R. Moessner, M.
Stone, D, Pajerowski, A. Samarakoon, D. A. Tennant, B. Winn, J.-
Q. Yan, Y. Yiu, S. Zhang.
Christian Balz
arXiv:1903.00056
Additional collaborators:
X. Hu, S. M. Yadav, Y. Takano
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4 SEN CNLS 2019
Outline
I. Kitaev’s model• Quick reminder of possible relevance to materials
• Basics of a-RuCl3
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5 SEN CNLS 2019
Kitaev’s model on honeycomb lattice – a special QSL
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6 SEN CNLS 2019
Kitaev’s model on honeycomb lattice – a special QSL
• Kitaev interaction: Bond-directional
dependent Ising coupling
• Exactly solvable Hamiltonian
→ quantum spin liquid ground state
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7 SEN CNLS 2019
Dynamics of Kitaev QSL
Majorana: a = a† ~ (f + f†)
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8 SEN CNLS 2019
Kitaev interactions in materials
d5 in low spin
octahedral
configuration
edge-sharing
octahedra
strong spin-
orbit coupling
See also:
H. Takagi et al.,
Nature Reviews Physics 1, (2019)
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9 SEN CNLS 2019
Heisenberg – Kitaev Phase Diagram
K
J
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10 SEN CNLS 2019
=
Effect of additional interactions
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11 SEN CNLS 2019
a-RuCl3 : quasi - 2D honeycomb material
• Honeycomb lattice
• Ru3+ in octahedral low spin
• J1/2 → J3/2 transition 200 meV
Transition to zig-zag order at TN = 7 K
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12 SEN CNLS 2019
Field dependence of TN BC 7.3 T
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13 SEN CNLS 2019
Additional ordered phase 6 – 7.3 T
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14 SEN CNLS 2019
Evidence of fractionalization from thermal Hall ?
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15 SEN CNLS 2019
Outline
II. Some inelastic neutron scattering• Magnons and fractional excitations in INS
• Inelastic neutron scattering in a-RuCl3
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16 SEN CNLS 2019
KCuF3 – a one dimensional S=1/2 HAFC•Tetragonal structure
•Chains of Cu2+ ions along c axis
•“Orbitally ordered” • Heisenberg AF chains of
S=1/2 Cu2+ ions
• Inter-chain coupling
leads to 3D AF order at
TN = 39 K
• Above TN the response
follows that expected for
the isolated S=1/2 chain
– which is much different
from that predicted for
classical spins
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17 SEN CNLS 2019
Energy dependence of the response below TN
3 fold degenerate
2 fold degenerate
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18 SEN CNLS 2019
Expectations for spin waves in a zigzag state
• Dispersion minima at ordering wavevectors (M points)
• Low energy constant E slices show cone shaped dispersion surfaces
around the M points
• Less general, but true for Heisenberg-Kitaev model:
G points show flat modes sharp in energy
-1
-0.5
0
0.5
1
[K,-
K,0
]
0
5
10
-0.5 0 0.5-1
-0.5
0
0.5
1
[H,H,0]
[K,-
K,0
]
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19 SEN CNLS 2019
a-RuCl3 single crystal - INS
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20 SEN CNLS 2019
Experiment: G point signal inconsistent with SW
T = 5 K
T= 10 K
• At TN 7 K the spin waves disappear throughout the Brillouin zone
• Above TN the continuum near the G point persists
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21 SEN CNLS 2019
Q,T dependence of the continuum scattering
• circular column centered on H=K=0, extending to higher energies
• at low T, moderate energy SW peaks and column merge and scattering
resembles a six pointed star
• scattering persists to high T
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22 SEN CNLS 2019
How does field affect the magnetic excitations?
4.8 K 10.2 K
4.8 K 10.2 K
Npj Quantum Materials 3, 8 (2018).
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23 SEN CNLS 2019
Outline
III. Recent results• Higher fields and 3rd dimension
• Magnetocaloric effect and T- B phase diagram
C. Balz et al., arXiv:1903.00056
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24 SEN CNLS 2019
FLEXX triple-axis-spectrometer
K. Habicht et al., EPJ Web of Conferences 83, 03007
(2015)
monochromator analyzer
13.5 T superconducting cryomagnet
detectorneutron beam
sample
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25 SEN CNLS 2019
Constant Q scans, zero field
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26 SEN CNLS 2019
Constant Q scans, B > 7.3 T
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27 SEN CNLS 2019
Constant Q scans, B > 9 T
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28 SEN CNLS 2019
Dispersion along L
Takeaway:
L dependence
consistent with
antiferromagnetic
interlayer
interaction (unit cell
has 3 layers)
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29 SEN CNLS 2019
Recall B dependence of line shape
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30 SEN CNLS 2019
B dependence of G point gap from INS
C. Balz et al.,
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31
Magnetocaloric Effect Y. Takano group
∆𝑇 ∝ −𝑇 𝜕𝑀
𝜕𝑇 𝐻∆𝐻
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32 SEN CNLS 2019
More complete phase diagram
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33 SEN CNLS 2019
Comparison with Kasahara et al. phase diagram
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34 SEN CNLS 2019
Some conclusions
• Inelastic neutron scattering in a-RuCl3 is
consistent with fractional excitations
• An external magnetic field applied in-plane leads
to a magnetically disordered state, with a higher
field transition to a state that seems to be
partially polarized and supports magnons
• The intermediate field state is consistent with a
QSL
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35 SEN CNLS 2019
References on a-RuCl3
Neutron scattering experiments:
• A. Banerjee et al. Nature Materials 15, 733(2016).
• H. Cao, A. Banerjee et al. PRB 93, 134423 (2016).
• A. Banerjee et al. SCIENCE 356, 1055 (2017).
• P. Lampen–Kelley et al. PRL 119, 237203, (2017).
• A. Banerjee et. al., Npj Quantum Materials 3, 8 (2018).
• C. Balz et al., arXiv:1903.00056
Others:
• M. Ziatdinov et al. Nat. Comm. 7, 13774 (2016).
• A. Samarakoon et al. PRB 96, 134408 (2017).
• A. Little et al. PRL 119, 227201 (2017).
• A. N. Ponomaryov et al., PRB 96, 241107(R), (2017).
• R. Hentrich et al., PRL 120, 117204 (2018).