Higgs Criticality in a two-dimensional metalqpt.physics.harvard.edu/talks/aps15.pdfAPS March...
Transcript of Higgs Criticality in a two-dimensional metalqpt.physics.harvard.edu/talks/aps15.pdfAPS March...
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HARVARD
APS March Meeting, San AntonioA14.00004
March 2, 2015
Debanjan Chowdhury and Subir Sachdev
Talk online: sachdev.physics.harvard.edu
Higgs Criticality in a two-dimensional metal
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Anti-ferromagnetwith p holesper square
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Anti-ferromagnetwith p holesper square
But relative to the band
insulator, there are 1+ p holesper square
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Strangemetal
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Strangemetal
Fermi liquid:Area enclosed
by Fermi surface =1+p
M. Plate, J. D. F. Mottershead, I. S. Elfimov, D. C. Peets, Ruixing Liang, D. A. Bonn, W. N. Hardy,S. Chiuzbaian, M. Falub, M. Shi, L. Patthey, and A. Damascelli, Phys. Rev. Lett. 95, 077001 (2005)
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Strangemetal
Pseudogap
“Fermi arcs” at
low p
Kyle M. Shen, F. Ronning, D. H. Lu, F. Baumberger, N. J. C. Ingle, W. S. Lee, W. Meevasana,Y. Kohsaka, M. Azuma, M. Takano, H. Takagi, Z.-X. Shen, Science 307, 901 (2005)
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A “Fractionalized Fermi liquid” (FL*) of holes of density p: has fermions
of spin S=1/2 and charge +e along with topological order in a background spin liquid
Strangemetal
R. K. Kaul, A. Kolezhuk, M. Levin, S. S., and T. Senthil, Phys. Rev. B 75, 235122 (2007)
Y. Qi and S. Sachdev, Phys. Rev. B 81, 115129 (2010)
D. Chowdhury and S. Sachdev, Phys. Rev. B 90, 245136 (2014).
M. Punk, A. Allais, and S. Sachdev, arXiv:1501.00978
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Strangemetal
Y. Kohsaka et al., Science 315, 1380 (2007)
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Y. Kohsaka et al., Science 315, 1380 (2007)
Q = (⇡/2, 0)x
y
d-form factor density wave order
M. A. Metlitski and S. Sachdev, Phys. Rev. B 82, 075128 (2010).S. Sachdev and R. LaPlaca, Phys. Rev. Lett. 111, 027202 (2013).
Predicted d form factor observedin STM measurements on BSCCO, Na-CCOC
K. Fujita, M. H Hamidian, S. D. Edkins, Chung Koo Kim, Y. Kohsaka, M. Azuma, M. Takano, H. Takagi,
H. Eisaki, S. Uchida, A. Allais, M. J. Lawler, E.-A. Kim, S. Sachdev, and J. C. Davis, PNAS 111, E3026 (2014)
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Y. Kohsaka et al., Science 315, 1380 (2007)
Q = (⇡/2, 0)x
y
d-form factor density wave order
Predicted d form factor observedin STM measurements on BSCCO, Na-CCOC
M. A. Metlitski and S. Sachdev, Phys. Rev. B 82, 075128 (2010).S. Sachdev and R. LaPlaca, Phys. Rev. Lett. 111, 027202 (2013).
K. Fujita, M. H Hamidian, S. D. Edkins, Chung Koo Kim, Y. Kohsaka, M. Azuma, M. Takano, H. Takagi,
H. Eisaki, S. Uchida, A. Allais, M. J. Lawler, E.-A. Kim, S. Sachdev, and J. C. Davis, PNAS 111, E3026 (2014)
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Q = (⇡/2, 0)
Strangemetal
D. Chowdhury and S. Sachdev,
Phys. Rev. B 90, 245136 (2014).
d-form factor density wave arises an instability of FL*
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Strangemetal
Sudden change in Fermi surface, as observed by STM, at optimal doping.
Apparent transition from p fermionic
quasiparticles to 1+p quasiparticles
Y. He et al., Science 344, 608-611 (2014)K. Fujita et al., Science 344, 612-616 (2014)
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Fermi surface+antiferromagnetism
+
Metal with “large” Fermi surface
The electron spin polarization obeys
D~S(r, ⌧)
E= ~'(r, ⌧)eiK·r
where K = (⇡,⇡) is the ordering
wavevector.
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s
1/g
Increasing SDW order
ConventionalFermi liquids
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electrons
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s
1/g(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electronsIncreasing SDW order
ConventionalFermi liquids
Hertz-Milliscriticality
of AFM order
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s
1/g
Increasing SDW order
(C) U(1) ACL with small holon pockets
ConventionalFermi liquids
Hertz-Milliscriticality
of AFM order
Non-Fermi liquid
M
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electrons
R. K. Kaul, A. Kolezhuk, M. Levin, S. Sachdev,
and T. Senthil, Phys. Rev. B 75, 235122 (2007).
Y. Qi and S. Sachdev, Phys. Rev. B 81, 115129 (2010).
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s
1/g
Increasing SDW order
(C) U(1) ACL with small holon pockets
ConventionalFermi liquids
Hertz-Milliscriticality
of AFM order
Non-Fermi liquid
M
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electrons
FL* forms by binding of holons
and spinons R. K. Kaul, A. Kolezhuk, M. Levin, S. Sachdev,
and T. Senthil, Phys. Rev. B 75, 235122 (2007).
Y. Qi and S. Sachdev, Phys. Rev. B 81, 115129 (2010).
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s
1/g
Increasing SDW order
(C) U(1) ACL with small holon pockets
ConventionalFermi liquids
Hertz-Milliscriticality
of AFM order
Non-Fermi liquids
FL* forms by binding of holons
and spinons
M
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu,
Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electrons
(D) SU(2) ACL with large Fermi surfaceof spinless fermions
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s
1/g
Increasing SDW order
(C) U(1) ACL with small holon pockets
(D) SU(2) ACL with large Fermi surfaceof spinless fermions
ConventionalFermi liquids
Hertz-Milliscriticality
of AFM order
Non-Fermi liquids
Higgscriticality
with no order parameter
M
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu,
Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surface of electrons
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Write the electron operator c↵ (↵ =", # are spin indices)
as
✓c"c#
◆= R
✓ +
�
◆
where R is a SU(2) matrix which determines the orienta-
tion of the local antiferromagnetic order, and ± are spin-
less fermions which carry the global electron U(1) charge.
This parameterization is invariant under a SU(2) gaugetransformation
✓ +
�
◆! U
✓ +
�
◆; R ! RU†
SU(2) gauge theory
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
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Assume field R is non-critical.
• Fermion , transforming as a gauge SU(2) fun-damental, with dispersion "k from the band struc-ture, at a non-zero chemical potential: has a“large” Fermi surface.
• A SU(2) gauge boson.
• A real Higgs field, H, transforming as a gaugeSU(2) adjoint, carrying lattice momentum (⇡,⇡).Condensation of the Higgs breaks SU(2)!U(1),and transforms the large Fermi surface to a smallFermi surface.
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
SU(2) gauge theory
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Assume field R is non-critical.
• Fermion , transforming as a gauge SU(2) fun-damental, with dispersion "k from the band struc-ture, at a non-zero chemical potential: has a“large” Fermi surface.
• A SU(2) gauge boson.
• A real Higgs field, H, transforming as a gaugeSU(2) adjoint, carrying lattice momentum (⇡,⇡).Condensation of the Higgs breaks SU(2)!U(1),and transforms the large Fermi surface to a smallFermi surface.
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
SU(2) gauge theory
The electrons, c↵ move in the presence of local antiferromag-
netic order ~n. In the rotating reference frame, this is equiv-
alent to a Yukawa coupling between the fermions and a
spin-singlet, gauge-SU(2) adjoint Higgs field Hagiven by
Ha=
1
2
Tr
⇥�`R�aR†⇤ n`
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Assume field R is non-critical.
• Fermion , transforming as a gauge SU(2) fun-damental, with dispersion "k from the band struc-ture, at a non-zero chemical potential: has a“large” Fermi surface.
• A SU(2) gauge boson.
• A real Higgs field, H, transforming as a gaugeSU(2) adjoint, carrying lattice momentum (⇡,⇡).Condensation of the Higgs breaks SU(2)!U(1),and transforms the large Fermi surface to a smallFermi surface.
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
SU(2) gauge theory
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SU(2) gauge theory for underlying quantum critical point
• The quantum critical theory is the Higgs transi-tion where the gauge “symmetry” breaks fromSU(2) down to U(1), in the presence of a Fermisurface of fermions carrying fundamental SU(2)charges.
• The Higgs condensation does not give the fermionsa “mass”; instead it reconstructs the Fermi sur-face from large to small.
• The quantum phase transition has no gauge-invariant “order parameter”, and it does notbreak any global symmetries.
s
(C) U(1) ACL with small holon pockets
(D) SU(2) ACL with large Fermi surface
Higgscriticality
with no order parameter
hRi = 0, hHai = 0hRi = 0, hHai 6= 0
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu,
Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
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SU(2) gauge theory for underlying quantum critical point
• The quantum critical theory is the Higgs transi-tion where the gauge “symmetry” breaks fromSU(2) down to U(1), in the presence of a Fermisurface of fermions carrying fundamental SU(2)charges.
• The Higgs condensation does not give the fermionsa “mass”; instead it reconstructs the Fermi sur-face from large to small.
• The quantum phase transition has no gauge-invariant “order parameter”, and it does notbreak any global symmetries.
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
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SU(2) gauge theory for underlying quantum critical point
• The quantum critical theory is the Higgs transi-tion where the gauge “symmetry” breaks fromSU(2) down to U(1), in the presence of a Fermisurface of fermions carrying fundamental SU(2)charges.
• The Higgs condensation does not give the fermionsa “mass”; instead it reconstructs the Fermi sur-face from large to small.
• The quantum phase transition has no gauge-invariant “order parameter”, and it does notbreak any global symmetries.
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
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Higgs transition between non-Fermi liquid metals with large and small Fermi surfaces
s
(C) U(1) ACL with small holon pockets
hRi = 0, hHai = 0hRi = 0, hHai 6= 0
Higgscriticality
with no order parameter S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu,
Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
Non-Fermi liquids
(D) SU(2) ACL with large Fermi surfaceof spinless fermions
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s
1/g
(A)AFM order with small Fermi pockets of electrons
(B) Fermi liquid with large Fermi surfaceof electrons
(C) U(1) ACL with small holon pockets
Hertz-Milliscriticality
of AFM order
Higgscriticality
with no order parameter
M
hRi = 0, hHai = 0
hRi 6= 0, hHai = 0hRi 6= 0, hHai 6= 0
hRi = 0, hHai 6= 0
Obtain conventional phases by condensing R
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu,
Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
ConventionalFermi liquids
Non-Fermi liquids
(D) SU(2) ACL with large Fermi surfaceof spinless fermions
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T **
U(1) FL* FL
T *
SU(2) ACL
AF
T
U(1) ACL
xd-BDW
Higgs QCP
SC
SU(2) gauge theory for underlying quantum critical point
S. Sachdev, M. A. Metlitski, Y. Qi, and C. Xu, Phys. Rev. B 80, 155129 (2009)
D. Chowdhury and S. Sachdev, arXiv:1412.1086
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Transport in QC regime:
All points on the Fermi surface have a rapid relaxation to local thermal
equilibrium by processes which conserve a suitably defined momentum.
Relaxation of the momentum occurs at a slower rate.
SU(2) gauge theory for underlying quantum critical point
S. A. Hartnoll, R. Mahajan, M. Punk and S. Sachdev, Phys. Rev. B 89, 155130 (2014)A. Patel and S. Sachdev, arXiv:1408.6549
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SU(2) gauge theory for underlying quantum critical point
The resistivity of this strange metal is not
determined by the scattering rate of charged
excitations near the Fermi surface, but by the
dominant rate of momentum loss by any
excitation, whether neutral or charged, or
fermionic or bosonic.
There is a dominant contribution ⇢(T ) ⇠ T by
the coupling of long-wavelength disorder to the
gauge-invariant operator O ⇠ H2.
S. A. Hartnoll, R. Mahajan, M. Punk and S. Sachdev, Phys. Rev. B 89, 155130 (2014)A. Patel and S. Sachdev, arXiv:1408.6549
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Conclusions1. Predicted d-form factor density wave order
observed in the non-La hole-doped cuprate superconductors.
2. Sudden change in Fermi surface, as observed by STM, at optimal doping: apparent transition from p fermionic quasiparticles to 1+p quasiparticles
3. Proposed a Higgs transition at optimal doping: involves change in Fermi surface and topological order, but has no order parameter.