Title: Subir Sachdev
1Loss of Neel order in insulators and
superconductors
Cenke Xu
Ribhu Kaul
Max Metlitski
Subir Sachdev arXiv0804.1794
2Phase diagram of electron-doped superconductors
3Spin correlations in the electron-doped
high-transition-temperature superconductor
Nd2-xCexCuO4 E. M. Motoyama, G. Yu, I. M. Vishik,
O. P. Vajk, P. K. Mang and M. Greven Nature 445,
186-189(11 January 2007)
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5Photoemission in NCCO
N. P. Armitage et al., Phys. Rev. Lett. 88,
257001 (2002).
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8Nature 450, 533 (2007)
9Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
10Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
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14Coupled dimer antiferromagnet
M. Matsumoto, C. Yasuda, S. Todo, and H.
Takayama, Phys. Rev.B 65, 014407 (2002).
15Square lattice antiferromagnet
Ground state has long-range Néel order
16Square lattice antiferromagnet
Destroy Neel order by perturbations which
preserve full square lattice symmetry e.g.
second-neighbor or ring exchange.
17Square lattice antiferromagnet
Destroy Neel order by perturbations which
preserve full square lattice symmetry e.g.
second-neighbor or ring exchange.
18Theory for loss of Neel order
19Perturbation theory
20Perturbation theory
Distinct universality from O(3) model
21Non-perturbative effects
F. D. M. Haldane, Phys. Rev. Lett. 61, 1029
(1988).
22Half-odd-integer S
Loss of Neel order leads to a Valence Bond Solid
(VBS)
N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694
(1989).
23Odd integer S
Loss of Neel order leads to a (charge) nematic
N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694
(1989).
24Even integer S
Loss of Neel order leads to a state with no
broken symmetry
N. Read and S. Sachdev, Phys. Rev. Lett. 62, 1694
(1989).
25Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
26Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
27Hole dynamics in an antiferromagnet across a
deconfined quantum critical point, R. K. Kaul,
A. Kolezhuk, M. Levin, S. Sachdev, and T.
Senthil, Physical Review B 75 , 235122 (2007).
Algebraic charge liquids and the underdoped
cuprates, R. K. Kaul, Y. B. Kim, S. Sachdev, and
T. Senthil, Nature Physics 4, 28 (2008).
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31Conventional phases
AF Metal
32Conventional phases
AF d-wave superconductor
4 Dirac points ( 4 shadows)
33Conventional phases
AF d-wave superconductor
Fermions fully gapped
34Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
35Outline
1. Loss of Neel order in insulating square
lattice antiferromagnets
Distinct universality classes for half-integer,
odd integer, and even integer spin
S 2. Low energy theory for doped S1/2
antiferromagnets d-wave superconductivity 3.
Loss of Neel order in the d-wave superconductor
Same universality classes as in general S
insulators, leading to transitions
to a valence bond supersolid, a
nematic superconductor, or a vanilla
superconductor
36Loss of Neel order in AFM d-wave superconductor
Fermions fully gapped
37Perturbation theory
38Recall non-perturbative effects in insulator
F. D. M. Haldane, Phys. Rev. Lett. 61, 1029
(1988).
39Non-perturbative effects in superconductor
40Non-perturbative effects in superconductor
41Non-perturbative effects in superconductor
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43Non-perturbative effects in superconductor
Transitions match those found in insulators for
different S
44Loss of Neel order in AFM d-wave superconductor
with gapless fermions
4 Dirac points ( 4 shadows)
45Perturbation theory
R. K. Kaul, Y. B. Kim, S. Sachdev, and T.
Senthil, Nature Physics 4, 28 (2008)
46Non-perturbative effects in superconductor
47Conclusions
- Theory for the loss of Neel order in d-wave
superconductors - For superconductors with gapped Bogoliubov
quasiparticles, we found 3 distinct transitions,
to a valence bond supersolid, a nematic
superconductor, and a vanilla superconductor - These transitions in the compressible
superconductor of S1/2 electrons match the
classification of transitions in the
incompressible Mott insulator of general S spins.