Holography of compressible quantum statesqpt.physics.harvard.edu/talks/brown11.pdf · Holography of...
Transcript of Holography of compressible quantum statesqpt.physics.harvard.edu/talks/brown11.pdf · Holography of...
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Holography of compressible quantum states
HARVARD
New England String Meeting, Brown University, November 18, 2011
sachdev.physics.harvard.eduSaturday, November 19, 2011
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Liza Huijse Max Metlitski Brian Swingle
Saturday, November 19, 2011
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• Consider an infinite, continuum,
translationally-invariant quantum system with a glob-
ally conserved U(1) chargeQ (the “electron density”)
in spatial dimension d > 1.
• Describe zero temperature phases where d�Q�/dµ �=0, where µ (the “chemical potential”) which changes
the Hamiltonian, H, to H − µQ.
• Compressible systems must be gapless.
• Conformal systems are compressible in d = 1, but
not for d > 1.
Compressible quantum matter
Saturday, November 19, 2011
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• Consider an infinite, continuum,
translationally-invariant quantum system with a glob-
ally conserved U(1) chargeQ (the “electron density”)
in spatial dimension d > 1.
• Describe zero temperature phases where d�Q�/dµ �=0, where µ (the “chemical potential”) which changes
the Hamiltonian, H, to H − µQ.
• Compressible systems must be gapless.
• Conformal systems are compressible in d = 1, but
not for d > 1.
Compressible quantum matter
Saturday, November 19, 2011
![Page 5: Holography of compressible quantum statesqpt.physics.harvard.edu/talks/brown11.pdf · Holography of compressible quantum states HARVARD New England String Meeting, Brown University,](https://reader034.fdocuments.in/reader034/viewer/2022050314/5f76e48a4063a22e454ee15f/html5/thumbnails/5.jpg)
• Consider an infinite, continuum,
translationally-invariant quantum system with a glob-
ally conserved U(1) chargeQ (the “electron density”)
in spatial dimension d > 1.
• Describe zero temperature phases where d�Q�/dµ �=0, where µ (the “chemical potential”) which changes
the Hamiltonian, H, to H − µQ.
• Compressible systems must be gapless.
• Conformal systems are compressible in d = 1, but
not for d > 1.
Compressible quantum matter
Saturday, November 19, 2011
![Page 6: Holography of compressible quantum statesqpt.physics.harvard.edu/talks/brown11.pdf · Holography of compressible quantum states HARVARD New England String Meeting, Brown University,](https://reader034.fdocuments.in/reader034/viewer/2022050314/5f76e48a4063a22e454ee15f/html5/thumbnails/6.jpg)
• Consider an infinite, continuum,
translationally-invariant quantum system with a glob-
ally conserved U(1) chargeQ (the “electron density”)
in spatial dimension d > 1.
• Describe zero temperature phases where d�Q�/dµ �=0, where µ (the “chemical potential”) which changes
the Hamiltonian, H, to H − µQ.
• Compressible systems must be gapless.
• Conformal systems are compressible in d = 1, but
not for d > 1.
Compressible quantum matter
Saturday, November 19, 2011
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One compressible state is the solid (or “Wigner crystal” or “stripe”).
This state breaks translational symmetry.
Compressible quantum matter
Saturday, November 19, 2011
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Another familiar compressible state is the superfluid.
This state breaks the global U(1) symmetry associated with Q
Condensate of fermion pairs
Compressible quantum matter
Saturday, November 19, 2011
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Graphene
Saturday, November 19, 2011
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The only other familiar
compressible phase is a
Fermi Liquid with a
Fermi surface
Saturday, November 19, 2011
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The only other familiar
compressible phase is a
Fermi Liquid with a
Fermi surface
• The only low energy excitations are long-lived quasiparticlesnear the Fermi surface.
Saturday, November 19, 2011
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The only other familiar
compressible phase is a
Fermi Liquid with a
Fermi surface
• Luttinger relation: The total “volume (area)” A enclosedby the Fermi surface is equal to �Q�.
A
Saturday, November 19, 2011
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1. Field theory
1I. Holography
Exotic phases of compressible quantum matter
Saturday, November 19, 2011
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1. Field theory
1I. Holography
Exotic phases of compressible quantum matter
Saturday, November 19, 2011
![Page 15: Holography of compressible quantum statesqpt.physics.harvard.edu/talks/brown11.pdf · Holography of compressible quantum states HARVARD New England String Meeting, Brown University,](https://reader034.fdocuments.in/reader034/viewer/2022050314/5f76e48a4063a22e454ee15f/html5/thumbnails/15.jpg)
ABJM theory in D=2+1 dimensions
• 4N2 Weyl fermions carrying fundamental chargesof U(N)×U(N)×SU(4)R.
• 4N2 complex bosons carrying fundamentalcharges of U(N)×U(N)×SU(4)R.
• N = 6 supersymmetry
Saturday, November 19, 2011
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ABJM theory in D=2+1 dimensions
• 4N2 Weyl fermions carrying fundamental chargesof U(N)×U(N)×SU(4)R.
• 4N2 complex bosons carrying fundamentalcharges of U(N)×U(N)×SU(4)R.
• N = 6 supersymmetry
Adding a chemical potential coupling to a SU(4) charge breaks supersymmetry and SU(4) invariance
Saturday, November 19, 2011
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• U(1) gauge invariance and U(1) global symme-try
• Fermions, f+ and f− (“quarks”), carry U(1)gauge charges ±1, and global U(1) charge 1.
• Bosons, b+ and b− (“squarks”), carry U(1) gaugecharges ±1, and global U(1) charge 1.
• No supersymmetry
• Fermions, c (“mesinos”), gauge-invariant boundstates of fermions and bosons carrying globalU(1) charge 2.
Theory similar to ABJM
L. Huijse and S. Sachdev, Physical Review D 84, 026001 (2011).Saturday, November 19, 2011
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Theory similar to ABJM
L. Huijse and S. Sachdev, Physical Review D 84, 026001 (2011).
• U(1) gauge invariance and U(1) global symme-try
• Fermions, f+ and f− (“quarks”), carry U(1)gauge charges ±1, and global U(1) charge 1.
• Bosons, b+ and b− (“squarks”), carry U(1) gaugecharges ±1, and global U(1) charge 1.
• No supersymmetry
• Fermions, c (“mesinos”), gauge-invariant boundstates of fermions and bosons carrying globalU(1) charge 2.
Saturday, November 19, 2011
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Theory similar to ABJM
L = f†σ
�(∂τ − iσAτ )−
(∇− iσA)2
2m− µ
�fσ
+ b†σ
�(∂τ − iσAτ )−
(∇− iσA)2
2mb+ �1 − µ
�bσ
+u
2
�b†σbσ
�2 − g1�b†+b
†−f−f+ +H.c.
�
+ c†�∂τ − ∇2
2mc+ �2 − 2µ
�c
−g2�c† (f+b− + f−b+) + H.c.
�
The index σ = ±1, and �1,2 are tuning parameters of phase diagram
Q = f†σfσ + b†σbσ + 2c†c
L. Huijse and S. Sachdev, Physical Review D 84, 026001 (2011).Saturday, November 19, 2011
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Theory similar to ABJM
L = f†σ
�(∂τ − iσAτ )−
(∇− iσA)2
2m− µ
�fσ
+ b†σ
�(∂τ − iσAτ )−
(∇− iσA)2
2mb+ �1 − µ
�bσ
+u
2
�b†σbσ
�2 − g1�b†+b
†−f−f+ +H.c.
�
+ c†�∂τ − ∇2
2mc+ �2 − 2µ
�c
−g2�c† (f+b− + f−b+) + H.c.
�
The index σ = ±1, and �1,2 are tuning parameters of phase diagram
Conserved U(1) charge: Q = f†σfσ + b†σbσ + 2c†c
L. Huijse and S. Sachdev, Physical Review D 84, 026001 (2011).Saturday, November 19, 2011
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Fermi liquid (FL) with Fermi surface of gauge-neutral mesinos
U(1) gauge theory is in confining phase
2Ac = �Q�
Ac
Phases of ABJM-like theories
�b±� = 0
Saturday, November 19, 2011
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Phases of ABJM-like theories
Af�b±� = 0
2Af = �Q�non-Fermi liquid (NFL)
with Fermi surface of gauge-charged quarksU(1) gauge theory is in deconfined phase
Saturday, November 19, 2011
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Phases of ABJM-like theories
Af�b±� = 0
S.-S. Lee, Phys. Rev. B 80, 165102 (2009)M. A. Metlitski and S. Sachdev, Phys. Rev. B 82, 075127 (2010)
Fermi surface coupled to Abelian or non-Abelian gauge fields:
• Longitudinal gauge fluctuations are screened by the fermions.
• Transverse gauge fluctuations are unscreened, and Landau-damped.They are IR fluctuations with dynamic critical exponent z > 1.
• Theory is strongly coupled in two spatial dimensions.
• “Non-Fermi liquid” broadening of the fermion quasiparticle pole.
Saturday, November 19, 2011
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Phases of ABJM-like theories
Af�b±� = 0
2Af = �Q�non-Fermi liquid (NFL)
with Fermi surface of gauge-charged quarksU(1) gauge theory is in deconfined phase
Saturday, November 19, 2011
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Phases of ABJM-like theories
Af�b±� = 0
2Af = �Q�
“Hidden” Fermi surface
non-Fermi liquid (NFL)with Fermi surface of gauge-charged quarks
U(1) gauge theory is in deconfined phase
Saturday, November 19, 2011
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2Ac + 2Af = �Q�
Phases of ABJM-like theories
�b±� = 0 AfAc
Fractionalized Fermi liquid (FL*)with Fermi surfaces of both quarks and mesinos
U(1) gauge theory is in deconfined phase
Saturday, November 19, 2011
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Fractionalized Fermi liquid (FL*)with Fermi surfaces of both quarks and mesinos
U(1) gauge theory is in deconfined phase
2Ac + 2Af = �Q�
Phases of ABJM-like theories
�b±� = 0 AfAc
Saturday, November 19, 2011
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Fractionalized Fermi liquid (FL*)with Fermi surfaces of both quarks and mesinos
U(1) gauge theory is in deconfined phase
2Ac + 2Af = �Q�
Phases of ABJM-like theories
�b±� = 0 AfAc
“Hidden” and visible Fermi surfaces co-exist
Saturday, November 19, 2011
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How do we detect the “hidden Fermi surfaces”
of fermions with gauge charges in the non-Fermi liquid phases ?
These are not directly visible in the gauge-invariant fermion correlations
computable via holography
Key question:
Saturday, November 19, 2011
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How do we detect the “hidden Fermi surfaces”
of fermions with gauge charges in the non-Fermi liquid phases ?
Compute entanglement entropy
One promising answer:
N. Ogawa, T. Takayanagi, and T. Ugajin, arXiv:1111.1023L. Huijse, B. Swingle, and S. Sachdev to appear.
Saturday, November 19, 2011
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B
A
Entanglement entropy of Fermi surfaces
ρA = TrBρ = density matrix of region A
Entanglement entropy SEE = −Tr (ρA ln ρA)
Saturday, November 19, 2011
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Logarithmic violation of “area law”: SEE =1
12(kFP ) ln(kFP )
for a circular Fermi surface with Fermi momentum kF ,where P is the perimeter of region A with an arbitrary smooth shape.
Non-Fermi liquids have, at most, the “1/12” prefactor modified.
B
A
Entanglement entropy of Fermi surfaces
D. Gioev and I. Klich, Physical Review Letters 96, 100503 (2006)B. Swingle, Physical Review Letters 105, 050502 (2010)
Saturday, November 19, 2011
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Logarithmic violation of “area law”: SEE =1
12(kFP ) ln(kFP )
for a circular Fermi surface with Fermi momentum kF ,where P is the perimeter of region A with an arbitrary smooth shape.
Non-Fermi liquids have, at most, the “1/12” prefactor modified.
B
A
Entanglement entropy of Fermi surfaces
Y. Zhang, T. Grover, and A. Vishwanath, Physical Review Letters 107, 067202 (2011)Saturday, November 19, 2011
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1. Field theory
1I. Holography
Exotic phases of compressible quantum matter
Saturday, November 19, 2011
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1. Field theory
1I. Holography
Exotic phases of compressible quantum matter
Saturday, November 19, 2011
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Begin with a CFT
Dirac fermions + gauge field + ......
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Holographic representation: AdS4
S =
�d4x
√−g
�1
2κ2
�R+
6
L2
��
A 2+1 dimensional
CFTat T=0
Saturday, November 19, 2011
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Apply a chemical potential to the “deconfined” CFT
Saturday, November 19, 2011
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+
++
++
+Electric flux
�Q��= 0
S =
�d4x
√−g
�1
2κ2
�R+
6
L2
�− 1
4e2FabF
ab
�
The Maxwell-Einstein theory of the applied chemical potential yields a AdS4-Reissner-Nordtröm black-brane
S. A. Hartnoll, P. K. Kovtun, M. Müller, and S. Sachdev, Physical Review B 76, 144502 (2007)
Er = �Q�Er = �Q�
r
Saturday, November 19, 2011
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+
++
++
+Electric flux
�Q��= 0
The Maxwell-Einstein theory of the applied chemical potential yields a AdS4-Reissner-Nordtröm black-brane
At T = 0, we obtain an extremal black-brane, witha near-horizon (IR) metric of AdS2 ×R2
ds2 =L2
6
�−dt2 + dr2
r2
�+ dx2 + dy2
r
Saturday, November 19, 2011
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Artifacts of AdS2 X R2
T. Faulkner, H. Liu, J. McGreevy, and D. Vegh, arXiv:0907.2694S. Sachdev, Phys. Rev. Lett. 105, 151602 (2010).
• Non-zero entropy density at T = 0
• Green’s function of a probe fermion (a mesino) canhave a Fermi surface, but self energies are momentumindependent, and the singular behavior is the sameon and off the Fermi surface
• Deficit of order ∼ N2 in the volume enclosed by themesino Fermi surfaces: presumably associated with“hidden Fermi surfaces” of gauge-charged particles(the quarks).
Saturday, November 19, 2011
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Holographic theory of a non-Fermi liquid (NFL)
Add a relevant “dilaton” field
Electric flux
C. Charmousis, B. Gouteraux, B. S. Kim, E. Kiritsis and R. Meyer, JHEP 1011, 151 (2010).
S. S. Gubser and F. D. Rocha, Phys. Rev. D 81, 046001 (2010).
N. Iizuka, N. Kundu, P. Narayan and S. P. Trivedi, arXiv:1105.1162 [hep-th].
Er = �Q�
Er = �Q�
r
S =
�d4x
√−g
�1
2κ2
�R− 2(∇Φ)2 − V (Φ)
L2
�− Z(Φ)
4e2FabF
ab
�
with Z(Φ) = Z0eαΦ, V (Φ) = −V0eδΦ, as Φ → ∞.
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Holographic theory of a non-Fermi liquid (NFL)
r
Add a relevant “dilaton” field
Electric flux
Er = �Q�
Er = �Q�
C. Charmousis, B. Gouteraux, B. S. Kim, E. Kiritsis and R. Meyer, JHEP 1011, 151 (2010).
S. S. Gubser and F. D. Rocha, Phys. Rev. D 81, 046001 (2010).
N. Iizuka, N. Kundu, P. Narayan and S. P. Trivedi, arXiv:1105.1162 [hep-th].
Leads to metric ds2 = L2
�−f(r)dt2 + g(r)dr2 +
dx2 + dy2
r2
�
with f(r) ∼ r−γ , g(r) ∼ rβ as r → ∞.
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Holographic theory of a non-Fermi liquid (NFL)
With the choice of the exponents, α, δ, a large zooof NFL phases appear possible. But the fate of theLuttinger count of Fermi surfaces seems unclear.
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Holographic theory of a non-Fermi liquid (NFL)
Key idea:
N. Ogawa, T. Takayanagi, and T. Ugajin, arXiv:1111.1023
Restrict attention to those models in which there islogarithmic violation of area law in the entanglement
entropy. This restricts δ = −α/3 andg(r) ∼ constant, as r → ∞.
ds2 = L2
�−dt2
rγ+ dr2 +
dx2 + dy2
r2
�
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Holographic theory of a non-Fermi liquid (NFL)
Evidence for “hidden” Fermi surface:
SEE = F (α)(P√Q) ln(P
√Q)
where P is the perimeter of the entangling region, andF (α) is a known function of α only.
• The dependence on Q and the shape of the en-tangling region is just as expected for a Fermisurface.
L. Huijse, B. Swingle, and S. Sachdev to appear.Saturday, November 19, 2011
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Logarithmic violation of “area law”: SEE =1
12(kFP ) ln(kFP )
for a circular Fermi surface with Fermi momentum kF ,where P is the perimeter of region A with an arbitrary smooth shape.
Non-Fermi liquids have, at most, the “1/12” prefactor modified.
B
A
Entanglement entropy of Fermi surfaces
Y. Zhang, T. Grover, and A. Vishwanath, Physical Review Letters 107, 067202 (2011)
D. Gioev and I. Klich, Physical Review Letters 96, 100503 (2006)B. Swingle, Physical Review Letters 105, 050502 (2010)
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Holographic theory of a non-Fermi liquid (NFL)
Evidence for “hidden” Fermi surface:
L. Huijse, B. Swingle, and S. Sachdev to appear.
SEE = F (α)(P√Q) ln(P
√Q)
where P is the perimeter of the entangling region, andF (α) is a known function of α only.
• The dependence on Q and the shape of the en-tangling region is just as expected for a Fermisurface.
Saturday, November 19, 2011
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Holographic theory of a non-Fermi liquid (NFL) and a fractionalized Fermi liquid (FL*)
L. Huijse, B. Swingle, and S. Sachdev to appear.
• Adding probe fermions leads to a (visible) Fermisurface of “mesinos” as in a FL* phase, and aholographic entanglement entropy in which
Q → Q−Qmesinos.
So only the “hidden” Fermi surfaces of “quarks”are measured by the holographic minimal areaformula.
SEE = F (α)(P√Q) ln(P
√Q)
where P is the perimeter of the entangling region, andF (α) is a known function of α only.
Saturday, November 19, 2011
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Holographic theory of a non-Fermi liquid (NFL)
Electric flux
In a deconfined NFL phase, the metric extends to infinity (representing critical IR modes),
and all of the electric flux “leaks out”.
Er = �Q�
Er = �Q�
r
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+
+
+
+ ++ Electric flux
In a deconfined FL* phase, the metric extends to infinity, there is a mesino charge density in the bulk,
and only part of the electric flux “leaks out”.
Holographic theory of a fractionalized Fermi liquid (FL*)
Er = �Q�
r
Er = �Q�− �Qmesino�
Saturday, November 19, 2011
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++
+
+
+ +Electric flux
In a confining FL phase, the metric terminates, all of the mesino density is in the bulk spacetime,
and none of the electric flux “leaks out”.
Holographic theory of a Fermi liquid (FL)S. SachdevarXiv:1107.5321
Er = �Q�
r
Er = 0
Saturday, November 19, 2011
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++
+
+
+ +Electric flux
Gauss Law in the bulk⇔ Luttinger theorem on the boundary
S. SachdevarXiv:1107.5321Holographic theory of a Fermi liquid (FL)
Er = �Q�
r
Er = 0
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Consider QED4, with full quantum fluctuations,
S =
�d4x
√g
�1
4e2FabF
ab + i�ψΓMDMψ +mψψ
��.
in a metric which is AdS4 in the UV, and confining in the IR.A simple model
ds2 =1
r2(dr2 − dt2 + dx2 + dy2) , r < rm
with rm determined by the confining scale.
S. SachdevarXiv:1107.5321Holographic theory of a Fermi liquid (FL)
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Massive Dirac fermions at zero chemical potentialDispersion E�(k) =
�k2 +M2
�Masses M� ∼ 1/rm
Almost all previous holographic theories have considered thesituation where the spacing between the E�(k) vanishes, and
an infinite number of E�(k) are relevant.
1 2 3 4
!4
!2
0
2
4
S. SachdevarXiv:1107.5321
k
E�(k)
Holographic theory of a Fermi liquid (FL)
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1 2 3 4
!4
!2
0
2
4
S. SachdevarXiv:1107.5321
k
E�(k)
Holographic theory of a Fermi liquid (FL)
Massive Dirac fermions at zero chemical potentialDispersion E�(k) =
�k2 +M2
�Masses M� ∼ 1/rm
Almost all previous holographic theories have considered thesituation where the spacing between the E�(k) vanishes, and
an infinite number of E�(k) are relevant.
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S. SachdevarXiv:1107.5321
1 2 3 4
-4
-2
0
2
4Dispersion at µ = 0
Dispersion at µ > 0
Holographic theory of a Fermi liquid (FL)
The spectrum at non-zero chemical potential is determined byself-consistently solving the Dirac equation and Gauss’s law:
��Γ · �D +m
�Ψ� = E�Ψ� ; ∇rEr =
�
�
�d2k
4π2Ψ†
�(k, z)Ψ�(k, z)f(E�(k))
where E is the electric field, and f(E) is the Fermi functionSaturday, November 19, 2011
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• The confining geometry implies that all gauge and gravitonmodes are gapped (modulo Landau damping from the Fermisurface).
• We can apply standard many body theory results, treating thismulti-band system in 2 dimensions, like a 2DEG at a semicon-ductor surface.
• Integrating Gauss’s Law, we obtain
Er(boundary)− Er(IR) = A
But Er(boundary) = �Q�, by the rules of AdS/CFT. So weobtain the usual Luttinger theorem of a Landau Fermi liquid,
A = �Q�
provided Er(IR) = 0.
Holographic theory of a Fermi liquid (FL)S. SachdevarXiv:1107.5321
Saturday, November 19, 2011
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• The confining geometry implies that all gauge and gravitonmodes are gapped (modulo Landau damping from the Fermisurface).
• We can apply standard many body theory results, treating thismulti-band system in 2 dimensions, like a 2DEG at a semicon-ductor surface.
• Integrating Gauss’s Law, we obtain
Er(boundary)− Er(IR) = A
But Er(boundary) = �Q�, by the rules of AdS/CFT. So weobtain the usual Luttinger theorem of a Landau Fermi liquid,
A = �Q�
provided Er(IR) = 0.
S. SachdevarXiv:1107.5321Holographic theory of a Fermi liquid (FL)
Saturday, November 19, 2011
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• The confining geometry implies that all gauge and gravitonmodes are gapped (modulo Landau damping from the Fermisurface).
• We can apply standard many body theory results, treating thismulti-band system in 2 dimensions, like a 2DEG at a semicon-ductor surface.
• Integrating Gauss’s Law, we obtain
Er(boundary)− Er(IR) = A
But Er(boundary) = �Q�, by the rules of AdS/CFT. So weobtain the usual Luttinger theorem of a Landau Fermi liquid,
A = �Q�
provided Er(IR) = 0.
S. SachdevarXiv:1107.5321Holographic theory of a Fermi liquid (FL)
Saturday, November 19, 2011
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++
+
+
+ +Electric flux
Gauss Law in the bulk⇔ Luttinger theorem on the boundary
S. SachdevarXiv:1107.5321Holographic theory of a Fermi liquid (FL)
Er = �Q�
r
Er = 0
In a confining FL phase, the metric terminates, all of the mesino density is in the bulk spacetime,
and none of the electric flux “leaks out”.
Saturday, November 19, 2011
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Conclusions
Compressible quantum matter
Evidence for hidden Fermi surfaces in compressible states obtained for a class of holographic Einstein-Maxwell-dilaton theories. These theories describe a non-Fermi liquid (NFL) state of gauge theories at non-zero density.
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Conclusions
Compressible quantum matter
Evidence for hidden Fermi surfaces in compressible states obtained for a class of holographic Einstein-Maxwell-dilaton theories. These theories describe a non-Fermi liquid (NFL) state of gauge theories at non-zero density.
Fermi liquid (FL) state described by a confining holographic geometry
Saturday, November 19, 2011
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Evidence for hidden Fermi surfaces in compressible states obtained for a class of holographic Einstein-Maxwell-dilaton theories. These theories describe a non-Fermi liquid (NFL) state of gauge theories at non-zero density.
Fermi liquid (FL) state described by a confining holographic geometry
Hidden Fermi surfaces can co-exist with Fermi surfaces of mesinos, leading to a fractionalized Fermi liquid (FL*)
Conclusions
Compressible quantum matter
Saturday, November 19, 2011