Eliashberg theory
E9105
Eliashberg theory is an extension of BCS superconductivity that incorporates strong-coupling and frequency-dependent effects to more accurately describe real superconducting materials.
All labels observed (10)
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
superconductivity theory
ⓘ
theoretical framework ⓘ |
| accountsFor |
finite quasiparticle lifetime
ⓘ
mass renormalization ⓘ strong electron-phonon coupling ⓘ |
| aimsTo | provide more accurate description than BCS for real materials ⓘ |
| applicableTo | isotropic s-wave superconductors ⓘ |
| appliesTo |
conventional phonon-mediated superconductors
ⓘ
strong-coupling superconductors ⓘ |
| assumes |
Migdal approximation
ⓘ
phonon-mediated pairing interaction ⓘ |
| canBe | analytically continued to real frequencies ⓘ |
| captures |
deviations from BCS gap ratio
ⓘ
strong-coupling corrections to thermodynamic quantities ⓘ |
| comparesWith | McMillan formula for Tc ⓘ |
| describes | superconducting state ⓘ |
| developedBy | G. M. Eliashberg ⓘ |
| developedIn | 1960s ⓘ |
| domain |
finite temperature
ⓘ
imaginary frequency axis ⓘ |
| equations |
Eliashberg theory
self-linksurface differs
ⓘ
surface form:
Eliashberg equations
|
| extends | BCS theory ⓘ |
| field | condensed matter physics ⓘ |
| formalism |
Green’s function formalism
ⓘ
Matsubara frequency formalism ⓘ |
| frameworkType | self-consistent integral equations ⓘ |
| generalizes |
BCS theory of superconductivity
ⓘ
surface form:
BCS weak-coupling limit
|
| hasExtension |
anisotropic Eliashberg theory
ⓘ
multiband Eliashberg theory ⓘ |
| includes |
Coulomb pseudopotential μ*
ⓘ
frequency-dependent electron-phonon interaction ⓘ retardation effects ⓘ self-energy corrections ⓘ |
| influenced | strong-coupling superconductivity research ⓘ |
| namedAfter | Gennady Eliashberg ⓘ |
| predicts |
critical temperature
ⓘ
quasiparticle renormalization ⓘ superconducting energy gap ⓘ |
| reducesTo | BCS theory in weak-coupling limit ⓘ |
| relatedTo |
Fermi liquid theory
ⓘ
Eliashberg theory self-linksurface differs ⓘ
surface form:
Migdal–Eliashberg theory
|
| usedFor |
analysis of optical conductivity in superconductors
ⓘ
analysis of tunneling spectra ⓘ interpretation of isotope effect ⓘ quantitative description of real superconductors ⓘ |
| uses |
Eliashberg theory
self-linksurface differs
ⓘ
surface form:
Eliashberg function α²F(ω)
electron-phonon spectral function ⓘ |
Referenced by (16)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Eliashberg equations
this entity surface form:
Eliashberg function α²F(ω)
this entity surface form:
Migdal–Eliashberg theory
this entity surface form:
Migdal-Eliashberg theory
this entity surface form:
Eliashberg strong‑coupling equations
this entity surface form:
Migdal–Eliashberg theory
this entity surface form:
Eliashberg spectral function
this entity surface form:
Eliashberg theory of superconductivity
this entity surface form:
Eliashberg theory of superconductivity
this entity surface form:
Migdal–Eliashberg theory
this entity surface form:
Migdal–Eliashberg theory of superconductivity
this entity surface form:
Migdal–Eliashberg strong-coupling theory