leapfrog integrator

E898982

A leapfrog integrator is a symplectic numerical method for solving Hamiltonian dynamics that conserves energy well over long simulations, making it especially useful in physics and Hamiltonian Monte Carlo.

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Label Occurrences
leapfrog integrator canonical 1

Statements (48)

Predicate Object
instanceOf geometric numerical integrator
numerical integration method
symplectic integrator
advantageOver non‑symplectic integrators for long‑time Hamiltonian simulation
appliedTo separable Hamiltonians
approximates Hamiltonian flow
assumes Hamiltonian separable into kinetic and potential energy
comparedTo Runge–Kutta methods NERFINISHED
enables high acceptance rates in Hamiltonian Monte Carlo
hasAlternativeName Störmer–Verlet integrator NERFINISHED
leapfrog method NERFINISHED
hasOrder 2
hasProperty conditionally stable
explicit method
good long‑term energy conservation
second‑order accurate
symplectic
time‑reversible
volume‑preserving in phase space
hasStepStructure full‑step position update
half‑step momentum update
half‑step momentum update at end of step
isSpecialCaseOf partitioned Runge–Kutta method
second‑order symplectic Runge–Kutta–Nyström method
minimizes long‑term energy drift
numericalErrorType bounded energy error over long times
preserves phase‑space volume
symplectic structure
relatedTo Störmer–Verlet method NERFINISHED
Verlet integration NERFINISHED
position Verlet integrator NERFINISHED
velocity Verlet integrator NERFINISHED
requires choice of time step
tradeoff smaller time step improves accuracy but increases cost
typicalUseContext Bayesian computation
Markov chain Monte Carlo NERFINISHED
classical mechanics
computational physics
usedFor Hamiltonian Monte Carlo NERFINISHED
Hybrid Monte Carlo NERFINISHED
N‑body simulations in astrophysics
long‑time integration of Hamiltonian systems
molecular dynamics simulations
solving Hamiltonian dynamics
usedIn galactic dynamics simulations
lattice quantum chromodynamics simulations
planetary orbit integration
rigid‑body dynamics

Referenced by (1)

Full triples — surface form annotated when it differs from this entity's canonical label.

Hamiltonian Monte Carlo typicallyUses leapfrog integrator