Peierls substitution
E136242
Peierls substitution is a quantum mechanical method for incorporating the effects of an external electromagnetic field into the momentum of charged particles in lattice or solid-state systems.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Peierls substitution canonical | 2 |
How this entity was disambiguated
This entity first appeared as the object of triple T1190366 — 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: Peierls substitution Context triple: [Rudolf Peierls, notableIdea, Peierls substitution]
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A.
Pippard nonlocal theory
Pippard nonlocal theory is a refinement of superconductivity theory that introduces spatially nonlocal relations between current and electromagnetic fields to account for finite coherence length effects beyond the London model.
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B.
Eliashberg theory
Eliashberg theory is an extension of BCS superconductivity that incorporates strong-coupling and frequency-dependent effects to more accurately describe real superconducting materials.
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C.
Rayleigh–Schrödinger perturbation theory
Rayleigh–Schrödinger perturbation theory is a fundamental method in quantum mechanics for approximating the energies and states of a system by treating interactions as small corrections to an exactly solvable problem.
-
D.
London equations
The London equations are fundamental relations in superconductivity that describe how magnetic fields behave inside superconductors, capturing key features like the Meissner effect and zero electrical resistance.
-
E.
Herzberg–Teller approximation
The Herzberg–Teller approximation is a refinement in molecular spectroscopy that accounts for vibronic coupling by allowing electronic transition dipole moments to depend on nuclear coordinates, explaining intensity in otherwise forbidden transitions.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Peierls substitution Target entity description: Peierls substitution is a quantum mechanical method for incorporating the effects of an external electromagnetic field into the momentum of charged particles in lattice or solid-state systems.
-
A.
Pippard nonlocal theory
Pippard nonlocal theory is a refinement of superconductivity theory that introduces spatially nonlocal relations between current and electromagnetic fields to account for finite coherence length effects beyond the London model.
-
B.
Eliashberg theory
Eliashberg theory is an extension of BCS superconductivity that incorporates strong-coupling and frequency-dependent effects to more accurately describe real superconducting materials.
-
C.
Rayleigh–Schrödinger perturbation theory
Rayleigh–Schrödinger perturbation theory is a fundamental method in quantum mechanics for approximating the energies and states of a system by treating interactions as small corrections to an exactly solvable problem.
-
D.
London equations
The London equations are fundamental relations in superconductivity that describe how magnetic fields behave inside superconductors, capturing key features like the Meissner effect and zero electrical resistance.
-
E.
Herzberg–Teller approximation
The Herzberg–Teller approximation is a refinement in molecular spectroscopy that accounts for vibronic coupling by allowing electronic transition dipole moments to depend on nuclear coordinates, explaining intensity in otherwise forbidden transitions.
- F. None of above. chosen
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
quantum mechanical method
ⓘ
solid-state physics technique ⓘ theoretical physics concept ⓘ |
| actsOn |
crystal momentum of electrons
ⓘ
hopping terms in tight-binding Hamiltonians ⓘ |
| appliesTo |
electrons in solids
ⓘ
lattice systems ⓘ tight-binding models ⓘ |
| approximationType |
effective low-energy description
ⓘ
semi-classical approximation ⓘ |
| assumes | slowly varying electromagnetic fields on lattice scale ⓘ |
| basedOn | minimal coupling prescription ⓘ |
| captures |
effect of magnetic field via Peierls phase
ⓘ
orbital coupling of electrons to magnetic field ⓘ |
| category |
electromagnetic coupling method in lattices
ⓘ
quantum lattice modeling technique ⓘ |
| domain |
lattice gauge theory (effective, non-fundamental use)
ⓘ
theoretical modeling ⓘ |
| effect |
encodes magnetic flux through lattice plaquettes
ⓘ
introduces complex phase factors in hopping amplitudes ⓘ |
| field |
condensed matter physics
ⓘ
quantum mechanics ⓘ solid-state physics ⓘ |
| formalism |
replaces hopping t by t·exp(i phase from vector potential)
ⓘ
replaces momentum operator p by p − qA in lattice context ⓘ |
| historicalContext | introduced in early development of solid-state quantum theory ⓘ |
| limitations |
approximate for strong-field, short-wavelength regimes
ⓘ
less accurate for rapidly varying fields ⓘ |
| namedAfter | Rudolf Peierls ⓘ |
| purpose |
incorporate external electromagnetic field effects
ⓘ
modify particle momentum in a lattice ⓘ |
| relatedTo |
Aharonov–Bohm effect
ⓘ
surface form:
Aharonov–Bohm effect in lattices
gauge invariance ⓘ minimal coupling in continuum ⓘ vector potential of electromagnetic field ⓘ |
| usedFor |
describing electron dynamics in magnetic fields
ⓘ
introducing gauge fields in lattice Hamiltonians ⓘ modeling charged particles in periodic potentials ⓘ studying Bloch electrons in magnetic fields ⓘ studying Hofstadter butterfly spectrum ⓘ studying quantum Hall effects in lattice models ⓘ |
| usedIn |
modeling graphene in magnetic fields
ⓘ
modeling superconducting vortex lattices (effective lattice models) ⓘ modeling topological insulators on lattices ⓘ numerical simulations of lattice electrons in fields ⓘ |
| validIn |
non-relativistic quantum mechanics
ⓘ
tight-binding approximation ⓘ |
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Subject: Peierls substitution Description of subject: Peierls substitution is a quantum mechanical method for incorporating the effects of an external electromagnetic field into the momentum of charged particles in lattice or solid-state systems.
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.