Bardeen–Stephen model of flux flow in superconductors
E37417
The Bardeen–Stephen model of flux flow in superconductors is a theoretical framework that describes how magnetic vortices move and dissipate energy in type-II superconductors under applied currents and fields.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Bardeen–Stephen model of flux flow in superconductors canonical | 1 |
| Nozières–Vinen model of vortex motion | 1 |
| Theory of the Motion of Vortices in Superconductors | 1 |
Statements (45)
| Predicate | Object |
|---|---|
| instanceOf |
model in superconductivity
ⓘ
phenomenological theory ⓘ theoretical model ⓘ |
| appliesTo | type-II superconductors ⓘ |
| approximates | vortex core as a cylinder of normal metal ⓘ |
| approximationType | macroscopic, continuum description of vortices ⓘ |
| assumes |
Ohmic dissipation in the vortex core
ⓘ
normal core inside each vortex ⓘ normal-state like resistivity in the vortex core ⓘ steady-state vortex motion ⓘ uniform current distribution on scales larger than vortex spacing ⓘ |
| basedOn |
Ginzburg–Landau theory of superconductivity
ⓘ
surface form:
time-dependent Ginzburg–Landau theory (phenomenologically)
|
| category |
mixed-state transport theory
ⓘ
vortex dynamics model ⓘ |
| comparedWith |
Bardeen–Stephen model of flux flow in superconductors
self-linksurface differs
ⓘ
surface form:
Nozières–Vinen model of vortex motion
|
| coreIdea | vortex motion produces an effective resistivity due to normal electrons in the core ⓘ |
| describes |
energy dissipation due to vortex motion
ⓘ
flux flow ⓘ flux-flow resistivity ⓘ motion of Abrikosov vortices ⓘ viscous drag on vortices ⓘ |
| field |
condensed matter physics
ⓘ
superconductivity ⓘ |
| givesFormulaFor | flux-flow resistivity ρ_ff ≈ ρ_n (B / Hc2) ⓘ |
| influenced | later theories of vortex dynamics ⓘ |
| introducedBy |
John Bardeen
ⓘ
Michael Stephen ⓘ |
| neglects |
Hall effect of vortices
ⓘ
inertial effects of vortices ⓘ pinning of vortices ⓘ |
| predicts |
flux-flow resistivity proportional to magnetic field
ⓘ
linear current–voltage characteristics in the flux-flow regime ⓘ vortex viscosity coefficient ⓘ |
| publishedIn | Physical Review ⓘ |
| relates |
flux-flow resistivity to normal-state resistivity
ⓘ
vortex velocity to Lorentz force and viscous drag ⓘ |
| titleOfOriginalPaper |
Bardeen–Stephen model of flux flow in superconductors
self-linksurface differs
ⓘ
surface form:
Theory of the Motion of Vortices in Superconductors
|
| usedFor |
estimating vortex viscosity from experiments
ⓘ
interpreting transport measurements in the mixed state ⓘ modeling flux-flow resistive transitions ⓘ |
| usesConcept |
upper critical field Hc2
ⓘ
vortex core radius of order coherence length ⓘ |
| validInRegime |
moderate magnetic fields below Hc2
ⓘ
temperatures not too far below Tc ⓘ |
| yearProposed | 1965 ⓘ |
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.
Bardeen–Stephen model of flux flow in superconductors
→
titleOfOriginalPaper
→
Bardeen–Stephen model of flux flow in superconductors
self-linksurface differs
ⓘ
this entity surface form:
Theory of the Motion of Vortices in Superconductors
Bardeen–Stephen model of flux flow in superconductors
→
comparedWith
→
Bardeen–Stephen model of flux flow in superconductors
self-linksurface differs
ⓘ
this entity surface form:
Nozières–Vinen model of vortex motion