Feshbach projection formalism
E177025
The Feshbach projection formalism is a quantum mechanical method that partitions a system’s Hilbert space into subspaces to derive effective Hamiltonians and describe interactions with continua or eliminated degrees of freedom.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Feshbach projection formalism canonical | 1 |
| Feshbach resonance | 1 |
| Nakajima–Zwanzig projection formalism | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T1565471 — 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: Feshbach projection formalism Context triple: [Brillouin–Wigner perturbation theory, relatedTo, Feshbach projection formalism]
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A.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
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B.
Gross–Pitaevskii equation
The Gross–Pitaevskii equation is a nonlinear Schrödinger-type equation that describes the macroscopic wavefunction and dynamics of weakly interacting Bose gases at ultra-cold temperatures.
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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.
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D.
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.
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E.
Bose–Einstein condensate
A Bose–Einstein condensate is an exotic state of matter formed when a dilute gas of bosons is cooled to temperatures near absolute zero, causing a large fraction of the particles to occupy the same quantum state and behave as a single quantum entity.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Feshbach projection formalism Target entity description: The Feshbach projection formalism is a quantum mechanical method that partitions a system’s Hilbert space into subspaces to derive effective Hamiltonians and describe interactions with continua or eliminated degrees of freedom.
-
A.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
-
B.
Gross–Pitaevskii equation
The Gross–Pitaevskii equation is a nonlinear Schrödinger-type equation that describes the macroscopic wavefunction and dynamics of weakly interacting Bose gases at ultra-cold temperatures.
-
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.
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.
-
E.
Bose–Einstein condensate
A Bose–Einstein condensate is an exotic state of matter formed when a dilute gas of bosons is cooled to temperatures near absolute zero, causing a large fraction of the particles to occupy the same quantum state and behave as a single quantum entity.
- F. None of above. chosen
Statements (42)
| Predicate | Object |
|---|---|
| instanceOf |
projection operator technique
ⓘ
quantum mechanical method ⓘ theoretical physics formalism ⓘ |
| appliedTo |
compound nucleus formation
ⓘ
decay into continua ⓘ effective interaction derivation in many-body systems ⓘ nuclear reactions ⓘ open quantum systems ⓘ optical model of nuclear scattering ⓘ quantum impurity problems ⓘ resonance scattering ⓘ |
| characteristicFeature |
eliminates selected degrees of freedom
ⓘ
introduces energy-dependent effective interactions ⓘ leads to non-Hermitian effective Hamiltonians in open systems ⓘ partitions Hilbert space into complementary subspaces ⓘ |
| defines |
P-space
ⓘ
Q-space ⓘ |
| developedBy | Herman Feshbach ⓘ |
| field |
many-body physics
ⓘ
nuclear physics ⓘ quantum mechanics ⓘ scattering theory ⓘ |
| historicalPeriod | mid-20th century ⓘ |
| influenced |
effective field theory approaches in nuclear physics
ⓘ
modern open quantum system theory ⓘ |
| mathematicalStructure |
coupled equations for P-space and Q-space components
ⓘ
decomposition of identity into projection operators ⓘ |
| purpose |
derive effective Hamiltonians for a reduced subspace
ⓘ
describe coupling between discrete states and continua ⓘ integrate out irrelevant or inaccessible degrees of freedom ⓘ |
| relatedTo |
Feshbach projection formalism
self-linksurface differs
ⓘ
surface form:
Feshbach resonance
Green’s function methods ⓘ Löwdin partitioning ⓘ Feshbach projection formalism self-linksurface differs ⓘ
surface form:
Nakajima–Zwanzig projection formalism
optical potential ⓘ |
| usesConcept |
Hilbert spaces
ⓘ
surface form:
Hilbert space
bound states ⓘ continuum states ⓘ effective Hamiltonian ⓘ projection operator ⓘ resonance ⓘ subspace decomposition ⓘ |
How these facts were elicited
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Subject: Feshbach projection formalism Description of subject: The Feshbach projection formalism is a quantum mechanical method that partitions a system’s Hilbert space into subspaces to derive effective Hamiltonians and describe interactions with continua or eliminated degrees of freedom.
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.