Feynman checkerboard model
E3528
discrete-time path integral
lattice model
model in quantum field theory
model in theoretical physics
path integral formulation
quantum mechanical model
The Feynman checkerboard model is a path-integral-based lattice model introduced by Richard Feynman to illustrate and derive the behavior of relativistic quantum particles, particularly the Dirac equation in one spatial dimension.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Feynman checkerboard model canonical | 1 |
| Feynman chessboard model | 1 |
| Feynman path integral on a lattice | 1 |
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
discrete-time path integral
ⓘ
lattice model ⓘ model in quantum field theory ⓘ model in theoretical physics ⓘ path integral formulation ⓘ quantum mechanical model ⓘ |
| aimsToExplain |
connection between relativistic motion and spinor structure
ⓘ
emergence of the Dirac equation from discrete paths ⓘ |
| alsoKnownAs |
Feynman checkerboard model
ⓘ
surface form:
Feynman chessboard model
Feynman checkerboard model ⓘ
surface form:
Feynman path integral on a lattice
|
| appliesTo | Dirac particle in one spatial dimension ⓘ |
| assumes |
discrete spacetime lattice with lightlike links
ⓘ
particle moves only left or right at each time step ⓘ |
| basedOn | path integral formulation of quantum mechanics ⓘ |
| category |
Feynman diagrams and path integrals
ⓘ
lattice quantum field theory models ⓘ |
| coreMechanism | assigning amplitudes to corners where direction changes ⓘ |
| creator | Richard Feynman ⓘ |
| describes | relativistic quantum particle in 1+1 dimensions ⓘ |
| dimension | 1+1 ⓘ |
| field |
lattice field theory
ⓘ
mathematical physics ⓘ quantum field theory ⓘ quantum mechanics ⓘ relativistic quantum mechanics ⓘ |
| historicalContext | introduced in the context of path integrals for relativistic particles ⓘ |
| illustrates |
how spin-1/2 behavior can emerge from path sums
ⓘ
relativistic propagation at the speed of light with direction reversals ⓘ |
| influenced |
discrete models of relativistic quantum mechanics
ⓘ
later work on quantum walks ⓘ |
| limitBehavior | continuum limit reproduces the Dirac propagator in 1+1 dimensions ⓘ |
| mathematicalRepresentation | sum over lattice paths with complex weights ⓘ |
| pedagogicalUse |
teaching path integrals
ⓘ
teaching the Dirac equation in low dimensions ⓘ |
| relatedTo |
Dirac equation
ⓘ
Feynman path integral ⓘ Dirac equation ⓘ
surface form:
Weyl equation in 1+1 dimensions
discrete-time quantum walk ⓘ lattice Dirac fermions ⓘ sum-over-paths approach ⓘ |
| spatialDimension | 1 ⓘ |
| temporalDimension | 1 ⓘ |
| usedFor | derivation of the 1+1 dimensional Dirac equation ⓘ |
| usesConcept |
amplitudes associated with corners in paths
ⓘ
lattice discretization of spacetime ⓘ lightlike lattice paths ⓘ sum over histories ⓘ zigzag paths at speed of light ⓘ |
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Feynman chessboard model
this entity surface form:
Feynman path integral on a lattice