Space-Time Approach to Non-Relativistic Quantum Mechanics
By R. Feynman. 2005
3,266 citations recorded by the source corpus.
Subfields: Atomic and Molecular Physics, and Optics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/8a0a777742559d8a1d512e4e7e97a579147d2597
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In Atomic and Molecular Physics, and Optics
- Parampreet Singh
- Abhay Ashtekar
- Lukas M. Sieberer
- M. Buchhold
- D. Storvick
- Gregory V. Vereshchagin
- S. Xue
- George Yin
In Statistical and Nonlinear Physics
- Abhay Ashtekar
- Parampreet Singh
- D. Storvick
- M. Buchhold
- Gregory V. Vereshchagin
- S. Xue
- George Yin
- Robert Schrader
Citations in the corpus
- Feynman–Kac formulas for regime-switching jump diffusions and their applications (2015, methodology): “Since the early work of Feynman [13] and Kac [19], the Feynman-Kac formulas have been extended and generalized in different directions.”
- Dynamics of non-Markovian open quantum systems (2015, background): “The path integral representation, first derived by Feynman and Vernon Jr. (1963) and Feynman (1948), constitutes a very convenient framework for performing numerical simulations of quantum dynamics and equilibrium quantum statistical mechanics, considering real and imaginary time evolution…”
- Non-Abelian Anyons and Interferometry (2007, background): “This fact is laid bare in the path integral formalism [14] of quantum mechanics, where the physical interpretation as a “sum over paths” makes it clear that the propagator (evolution kernel) splits into contributions from homotopically inequivalent path sectors labeled by elements of π1 (CN).”
- Do We Really Understand Quantum Mechanics? (2012, methodology): “A point of comparison might be the theory of path integrals introduced by Feynman [51, 52], which is usually considered as a branch of standard quantum mechanics (§ 1.”
- Ramsey-type phase control of free-electron beams (2016, background): “ulting final state is composed of a superposition of momentum sidebands associated with energy changes by ±N photon energies,25,26 populated with amplitudes A N according to 𝐴𝑁= ( 𝑔 |𝑔| ) 𝑁 𝐽𝑁(2|𝑔|), (1) where J N are the Nth-order Bessel functions. The dimensionless coupling parameter g des”
- Keldysh field theory for driven open quantum systems (2015, methodology): “In the first case, a real time path integral can be constructed along the lines of Feynman’s original path integral formulation of quantum mechanics [179].”
- Brownian motions on metric graphs (2011, methodology): “A complete description of the history is beyond the scope of this introduction, but in keywords we want to mention the following: The construction of Wiener space [89] and Wiener’s approach of statistical mechanics and chaos [90], Itô’s theory of stochastic integration [39] and stochastic differenti”
- A Survey of Results Involving Transforms and Convolutions in Function Space (2004, background): “Feynman [25] obtained such functionals by formally integrating out the oscillator coordinates in a system involving a harmonic oscillator interacting with a particle moving in a potential.”
- Geometrical Structure of Laplacian Eigenfunctions (2012, methodology): “This relation is also known as a semiclassical approximation in quantum mechanics and a ray approximation of wave propagation in optics, while the correspondence between classical and quantum systems can be shown using the WKB method, Eikonal equation, or Feynman path integrals [179, 180, 362].”
- Light Hadron Masses from Lattice QCD (2012, methodology): “We start by writing the partition function of a Euclidean quantum field theory using the path integral formalism (Dirac, 1933; Feynman, 1948a,b, 1949; Feynman 3 and Hibbs, 1965) as Z = ∫ DΦe−S(Φ) (1) with the action S(Φ) and Φ generically denoting all fields of the theory.”