Ehrenfest theorem
E735839
The Ehrenfest theorem is a fundamental result in quantum mechanics that links the time evolution of expectation values of quantum observables to the corresponding classical equations of motion, thereby bridging quantum and classical physics.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Ehrenfest theorem canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T8490717 — 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: Ehrenfest theorem Context triple: [Paul Ehrenfest, notableWork, Ehrenfest theorem]
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A.
Liouville–von Neumann equation
The Liouville–von Neumann equation is the fundamental quantum-mechanical evolution equation governing the time dependence of the density operator, generalizing the Schrödinger equation to mixed states and open-system dynamics.
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B.
Feynman–Hellmann theorem
The Feynman–Hellmann theorem is a result in quantum mechanics that relates the derivative of an energy eigenvalue with respect to a parameter in the Hamiltonian to the expectation value of the corresponding derivative of the Hamiltonian.
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C.
Schrödinger equation
The Schrödinger equation is the fundamental equation of non-relativistic quantum mechanics that governs how the quantum state of a physical system evolves over time.
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D.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
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E.
H-theorem
The H-theorem is Boltzmann’s foundational result in statistical mechanics that explains the irreversible increase of entropy in a gas from time-reversible microscopic dynamics, providing a key link between mechanics and the second law of thermodynamics.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Ehrenfest theorem Target entity description: The Ehrenfest theorem is a fundamental result in quantum mechanics that links the time evolution of expectation values of quantum observables to the corresponding classical equations of motion, thereby bridging quantum and classical physics.
-
A.
Liouville–von Neumann equation
The Liouville–von Neumann equation is the fundamental quantum-mechanical evolution equation governing the time dependence of the density operator, generalizing the Schrödinger equation to mixed states and open-system dynamics.
-
B.
Feynman–Hellmann theorem
The Feynman–Hellmann theorem is a result in quantum mechanics that relates the derivative of an energy eigenvalue with respect to a parameter in the Hamiltonian to the expectation value of the corresponding derivative of the Hamiltonian.
-
C.
Schrödinger equation
The Schrödinger equation is the fundamental equation of non-relativistic quantum mechanics that governs how the quantum state of a physical system evolves over time.
-
D.
Fokker–Planck equation
The Fokker–Planck equation is a partial differential equation that describes the time evolution of the probability density function of a stochastic (random) process, such as Brownian motion.
-
E.
H-theorem
The H-theorem is Boltzmann’s foundational result in statistical mechanics that explains the irreversible increase of entropy in a gas from time-reversible microscopic dynamics, providing a key link between mechanics and the second law of thermodynamics.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf | quantum mechanics theorem ⓘ |
| appliesTo |
expectation values
ⓘ
general Hermitian operators ⓘ momentum operator ⓘ position operator ⓘ quantum observables ⓘ |
| assumes |
self-adjoint operators for observables
ⓘ
sufficiently well-behaved wavefunctions ⓘ |
| bridges | quantum mechanics and classical mechanics ⓘ |
| canBeGeneralizedTo | relativistic quantum mechanics ⓘ |
| category | theorems in quantum mechanics ⓘ |
| clarifies | relationship between operator equations and classical laws ⓘ |
| concerns | expectation value dynamics ⓘ |
| describes | time evolution of expectation values of observables ⓘ |
| field | quantum mechanics ⓘ |
| hasDomain | nonrelativistic quantum mechanics ⓘ |
| hasFormula | d⟨A⟩/dt = (i/ħ)⟨[H,A]⟩ + ⟨∂A/∂t⟩ ⓘ |
| historicalPeriod | early 20th century ⓘ |
| holdsIn |
Heisenberg picture
NERFINISHED
ⓘ
Schrödinger picture NERFINISHED ⓘ |
| implies |
d⟨p⟩/dt = −⟨∂V/∂x⟩ for potential V(x)
ⓘ
d⟨x⟩/dt = ⟨p⟩/m for a particle of mass m ⓘ |
| importance | fundamental for understanding quantum–classical correspondence ⓘ |
| involves |
Hamiltonian operator
ⓘ
commutators ⓘ |
| isUsedFor |
connecting quantum dynamics to classical trajectories
ⓘ
interpretation of quantum motion ⓘ semiclassical analysis ⓘ |
| mathematicallyExpressedIn |
Hilbert space framework
ⓘ
operator formalism ⓘ |
| mayFailToGive | exact classical motion for highly nonclassical states ⓘ |
| namedAfter | Paul Ehrenfest NERFINISHED ⓘ |
| relatedTo |
Heisenberg equation of motion
NERFINISHED
ⓘ
Heisenberg uncertainty principle NERFINISHED ⓘ Schrödinger equation of motion NERFINISHED ⓘ correspondence principle ⓘ |
| relates |
quantum expectation values to classical equations of motion
ⓘ
time derivative of expectation value to commutator with Hamiltonian ⓘ |
| shows | classical equations emerge from quantum mechanics in expectation values ⓘ |
| specialCase | Newton’s second law in expectation value form ⓘ |
| typeOf | dynamical theorem ⓘ |
| usedIn |
atomic physics
ⓘ
condensed matter physics ⓘ molecular dynamics with quantum effects ⓘ quantum chemistry ⓘ |
| uses |
Heisenberg equation of motion
NERFINISHED
ⓘ
Schrödinger equation NERFINISHED ⓘ |
| validUnder | smooth potentials ⓘ |
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Subject: Ehrenfest theorem Description of subject: The Ehrenfest theorem is a fundamental result in quantum mechanics that links the time evolution of expectation values of quantum observables to the corresponding classical equations of motion, thereby bridging quantum and classical physics.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.