London theory of superconductivity
E243123
The London theory of superconductivity is a foundational phenomenological model that explains key electromagnetic properties of superconductors, such as perfect diamagnetism and the Meissner effect, through the London equations.
All labels observed (1)
| Label | Occurrences |
|---|---|
| London theory of superconductivity canonical | 2 |
How this entity was disambiguated
This entity first appeared as the object of triple T2173849 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: London theory of superconductivity Context triple: [Heinz London, notableWork, London theory of superconductivity]
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A.
BCS theory of superconductivity
The BCS theory of superconductivity is a fundamental microscopic theory that explains superconductivity through the formation of Cooper pairs of electrons and their collective quantum behavior in a solid.
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B.
Ginzburg–Landau theory of superconductivity
The Ginzburg–Landau theory of superconductivity is a phenomenological framework that describes superconductors using a complex order parameter and macroscopic equations to capture phase transitions, coherence length, and magnetic behavior.
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C.
Bardeen–Stephen model of flux flow in superconductors
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.
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D.
Schrieffer
Schrieffer is the surname of John Robert Schrieffer, the American physicist and Nobel laureate known for co-developing the BCS theory of superconductivity.
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E.
Abrikosov vortices
Abrikosov vortices are quantized magnetic flux lines that penetrate type-II superconductors in a regular lattice when exposed to magnetic fields above a critical value.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: London theory of superconductivity Target entity description: The London theory of superconductivity is a foundational phenomenological model that explains key electromagnetic properties of superconductors, such as perfect diamagnetism and the Meissner effect, through the London equations.
-
A.
BCS theory of superconductivity
The BCS theory of superconductivity is a fundamental microscopic theory that explains superconductivity through the formation of Cooper pairs of electrons and their collective quantum behavior in a solid.
-
B.
Ginzburg–Landau theory of superconductivity
The Ginzburg–Landau theory of superconductivity is a phenomenological framework that describes superconductors using a complex order parameter and macroscopic equations to capture phase transitions, coherence length, and magnetic behavior.
-
C.
Bardeen–Stephen model of flux flow in superconductors
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.
-
D.
Schrieffer
Schrieffer is the surname of John Robert Schrieffer, the American physicist and Nobel laureate known for co-developing the BCS theory of superconductivity.
-
E.
Abrikosov vortices
Abrikosov vortices are quantized magnetic flux lines that penetrate type-II superconductors in a regular lattice when exposed to magnetic fields above a critical value.
- F. None of above. chosen
Statements (44)
| Predicate | Object |
|---|---|
| instanceOf |
electromagnetic theory
ⓘ
phenomenological theory ⓘ theory of superconductivity ⓘ |
| appliesTo |
bulk superconducting materials
ⓘ
superconductors ⓘ |
| approximates | superconductors as perfect diamagnets ⓘ |
| assumes |
macroscopic quantum coherence of superconducting electrons
ⓘ
superconducting current proportional to vector potential ⓘ |
| basedOn | London equations ⓘ |
| characterizes |
magnetic field penetration in superconductors
ⓘ
superconducting current response to electromagnetic fields ⓘ |
| connectedTo | Maxwell equations in matter ⓘ |
| contrastsWith | microscopic BCS theory ⓘ |
| coreIdea | superconducting electrons move without resistance in response to electromagnetic fields ⓘ |
| countryOfOrigin | United Kingdom ⓘ |
| describes | electromagnetic properties of superconductors ⓘ |
| explains |
Meissner effect
ⓘ
perfect diamagnetism ⓘ |
| field |
condensed matter physics
ⓘ
theoretical physics ⓘ |
| formulatedBy |
Fritz London
ⓘ
Heinz London ⓘ |
| historicalSignificance | first successful phenomenological description of Meissner effect ⓘ |
| ignores | normal electron contribution in ideal limit ⓘ |
| influenced | development of Ginzburg–Landau theory ⓘ |
| inspired | subsequent gauge-invariant formulations of superconductivity ⓘ |
| introducesConcept | London penetration depth ⓘ |
| language | classical field equations ⓘ |
| mathematicalFormulation |
London equations
ⓘ
surface form:
first London equation
second London equation ⓘ |
| neglects | microscopic pairing mechanism ⓘ |
| precedes | BCS theory of superconductivity ⓘ |
| predicts |
exponential decay of magnetic field inside a superconductor
ⓘ
zero magnetic field in the bulk of an ideal superconductor ⓘ |
| relatedConcept |
flux expulsion
ⓘ
superconducting condensate ⓘ supercurrent density ⓘ |
| scope | linear response of superconductors to weak fields ⓘ |
| type | macroscopic theory ⓘ |
| usedFor |
estimating penetration depth from experimental data
ⓘ
modeling magnetic response of type I superconductors ⓘ |
| validInRegime |
length scales larger than coherence length
ⓘ
low-frequency electromagnetic fields ⓘ |
| yearProposed | 1935 ⓘ |
How these facts were elicited
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Subject: London theory of superconductivity Description of subject: The London theory of superconductivity is a foundational phenomenological model that explains key electromagnetic properties of superconductors, such as perfect diamagnetism and the Meissner effect, through the London equations.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.