what happens inside a unit cell matters – effect of umklapp … · 2013. 9. 13. · what happens...
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What Happens inside a Unit Cell Matters –
Effect of Umklapp Process
Wei-Cheng Lee
Department of Physics
University of Illinois at Urbana-Champaign
In collaboration with Anthony J. Leggett (UIUC)
This work is supported by Center for Emergent Superconductivity,
an Energy Frontier Research Center sponsored by DOE, USA.
Center for Emergent Superconductivity
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Energy Scales in Strongly Correlated Systems
meVU310:Charge ≈
meVJ 10:Magnetic 2≈
meVPairing 10 : 1≈∆
cBTk
cEEnergy on condensati
Theory BCS Still true in strongly
correlated systems?
meV010<
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MagnetismCDW
Nematicity ????Superconductivity
Fermi liquid
Groundstate Energy
Turn on interaction
~U
Why can superconductivity often win this battle in some range of phase diagram
in a variety of materials?
Any interaction that is much smaller but just enough to help superconductivity to
win?
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Energetic Consideration
Chester, Phys. Rev. 103, 1693 (1956)
Leggett’s extension:
Stronger Coulomb interaction (smaller ε) leads to larger superconducting condensation energy!!!
NsSNcond VVHHE
VKVVKH
ˆˆ0ˆˆ
Theorem) (Virial ˆ2
1ˆ , ˆ2
1 ˆˆˆ
<⇒>−=
−==+=
( ) 0ˆˆ1ˆˆ
change,can that parameter only theis If
cores ionic by the edrenormalizconstant dielectric , ... 4
1
2
1ˆ2
0
<−=∂
∂−
∂
∂=
∂
∂
=+−
= ∑
NssN
cond
ij ji
VVVVE
rr
eV
εεεε
ε
εεπε
rr
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Short Range Coulomb Interaction
Strongly correlated systems
Electrons need to rearrange themselves locally to compromise
the short range interaction
‘Extended’ description, e.g., band structure description, is likely
breaking down and new phases like AFM, nematicity, Mottness,
etc. can emerge.
How can superconductivity, a delocalized state, comprise the
short range interaction??
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Savings of Short Range Part of Coulomb Energy (Large q)
Coulomb Energy:
Superconducting condensation energy in this region:
Short Range Part of Coulomb Energy can be saved in
superconducting state by sign-changing gap function (for
example, d-wave in cuprates)
q
eU
q
eU
ccVUH
D
q
D
q
k
kqkq
q
q
q
qqqCoul
∞∞
+−
≠≠−
==
=Ω
≡Ω
= ∑∑∑
εεεε
ρρρσ
σσ
0
22
2
0
23
,
,,
00
2 ,
ˆ , ˆ2
1 ˆˆ
2
1
∑−+
−− ∆∆−≈−=k
qk
qk
qS
qqqN
qqqqC UUUVE2
*
2
)ˆ( ρρρρδ))))
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What about long-
range Coulomb
Energy?
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Some Arguments about the Long Range Part of Coulomb Energy
• Screening??
• 3D Yes, screening is effective.
• 2D Not necessary!!!
• Anderson’s theory (Phys. Rev. 110, 827(1958),
Phys. Rev. 112, 1900(1958))
• For small q, the plasma mode is still the only
excitation in superconducting state, and its
frequency is the same as the one in normal
state. No change in Long-ranged Coulomb
energy due to superconductivity.
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Unconventional Superconductors are
all built on 2D Lattice!!!
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Rigorous sum rules for density-density response function:
Applying Cauchy-Schwartz inequalities places limits on
the Coulomb Energy at small q
scattering Umklapp)ˆ(1
)(),(Im2
rule sum-f ),(Im2
relationKK )0,(),(Im2
2
4
2
24
2
2
0
3
3
2
01
01
∑
∫
∫
∫
−
∞
∞
∞
−
⋅Ω
−=
++=≡
=≡
==≡
k
kk
q
UqkA
qoVm
nqA
m
qqdJ
m
nqqdJ
dJ
ρπ
ωχωωπ
ωχωωπ
ωχω
ωχω
π
Role of Umklapp Scattering I Sum Rule Analysis
M. Turlakov and A.J. Leggett, Phys. Rev. B 67, 044517 (2003)
)(/1
1
2)(
2
2
2
2qo
nmAVqo
p
p
q
p+
+≥≥+
ω
ωω hh
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Take Away Message
Without periodic potential, plasmon mode is IMMORTAL at small q.
With periodic potential (Umklapp scattering), plasmon mode is no
longer IMMORTAL at small q.
MIR spectra
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Microscopic theory of the density-density correlation
function with Umklapp process
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Warm Up – Plasmon Excitation in
Fermi Liquid
Random phase approximation (RPA)
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Warm Up – Plasmon Excitation in
Fermi Liquid
p-h
continuumPlasmon
excitation!!!
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Periodic Potential
both have p-h continuum ~ q
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Generalized RPA with Umklapp
Process
p-h
continuum
New spectral weight in Mid Infrared region appears due to the Umklapp process!!!
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Why Plasmon Loses Spectral
Weight?
(a) No Umklapp process
(b) With Umklapp process
What happens inside a unit cell is the key!!!
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Calculations
To obtain a truly broad spectrum, we need to go beyond RPA.
Solving the Kinetic equations can do the trick.
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Why Superconductivity Can Take
Advantage?
Because it is not local and gapped, it has much less Umklapp
scattering!!!
Umklapp scattering Mid Infrared peaks increase long-ranged
Coulomb energy
Superconductivity suppresses Umklapp scattering Mid Infrared
peaks reduced long-ranged Coulomb energy decreased!!!
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Experimental Observation in
Cuprates
Mole graaf, et. al., Science 295, 2239 (2002)
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Experimental Observations in Iron
Pnictides
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Fermi Surface Consideration
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Umklapp scattering also affects
pairing interaction
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Final Remarks
Why superconductivity is so competitive?• Short-ranged Coulomb energy saved by sign-changing gap
• Long-ranged Coulomb energy saved by reducing Umklapp
process
• Higher Tc superconductivity might occur in materials with 2D
lattice, localized orbitals, and smaller dielectric constant.
Much more efforts should be spent on changes due to superconductivity on optical conductivity, electron energy loss spectroscopy (EELS)!!!