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Quantization (physics)

About: Quantization (physics) is a research topic. Over the lifetime, 20776 publications have been published within this topic receiving 562403 citations. The topic is also known as: quantisation.


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TL;DR: In this paper, a functional approach to scattering theory in quantum field theory is developed by deriving an explicit functional expression for transition amplitudes, which avoids noncommutativity problems of field operators, avoids solving the field equations, avoids dealing with the often quite complicated continual (path) integrals, and avoids combinatoric problems associated with Feynman rules and the old-fashioned Wick's theorem.
Abstract: A functional approach to scattering theory in quantum field theory is developed by deriving an explicit functional expression fortransition amplitudes. In applications, the formalism avoids dealing with noncommutativity problems of field operators, avoids solving the field equations, avoids dealing with the often quite complicated continual (path) integrals, and avoids combinatoric problems associated with Feynman rules and the old-fashioned Wick's theorem. Finally, it avoids explicitly taking mass shell limits as in the LSZ formalism. The basic idea of the formalism is to use the quantum action principle followed by a systematic analysis of the concept of stimulated emissions as applied to particles of any spin, and is a generalization of an earlier method applied by the author to the much simpler situation of quantum mechanics.

6 citations

Journal ArticleDOI
TL;DR: In this paper, the authors investigated the quantization of electromagnetic waves propagating through homogeneous conducting linear media with no charge density and used Coulomb's gauge to reduce the problem to that of a time-dependent harmonic oscillator, which is described by the Caldirola-Kanai Hamiltonian.
Abstract: In this work we investigate the quantization of electromagnetic waves propagating through homogeneous conducting linear media with no charge density. We use Coulomb's gauge to reduce the problem to that of a time-dependent harmonic oscillator, which is described by the Caldirola–Kanai Hamiltonian. Furthermore, we obtain the corresponding exact wave functions with the help of quadratic invariants and of the dynamic invariant method. These wave functions are written in terms of a particular solution of the Milne–Pinney equation. We also construct coherent and squeezed states for the quantized electromagnetic waves and evaluate the quantum fluctuations in coordinates and momentum as well as the uncertainty product for each mode of the electromagnetic field.

6 citations

Journal ArticleDOI
TL;DR: In this article, a general formalism is given inside quantum field theory to describe a macro system's separation from the surrounding and its time evolution, assuming a suitable dissipative behaviour of the time evolution of the separated system.
Abstract: For a macrosystem a general formalism is given, inside quantum field theory, to describe its separation from the surrounding and its time evolution. Assuming a suitable dissipative behaviour of the time evolution of the separated system, an objective quantum description is extracted from quantum field theory, based on a natural set of non-local hidden variables. In the non-relativistic case, compatibility with usual statistical mechanics is discussed in the context of a Boltzmann description; finally, the coherence is shown with the point of view of Bohr about quantum mechanics of a microsystem.

6 citations

Journal ArticleDOI
TL;DR: In this paper, a spinor model of a free massless spinning particle in 4-dimensional Minkowski space is studied in terms of spacetime and spinor variables, which is specified by a simple action referred to here as the gauged Shirafuji action, that consists of twistor variables and gauge fields on the 1-dimensional parameter space.
Abstract: A twistor model of a free massless spinning particle in 4-dimensional Minkowski space is studied in terms of spacetime and spinor variables. This model is specified by a simple action, referred to here as the gauged Shirafuji action, that consists of twistor variables and gauge fields on the 1-dimensional parameter space. We consider the canonical formalism of the model by following the Dirac formulation for constrained Hamiltonian systems. In the subsequent quantization procedure, we obtain a plane-wave solution with momentum spinors. From this solution and coefficient functions, we construct positive-frequency and negative-frequency spinor wave functions defined on complexified Minkowski space. It is shown that the Fourier-Laplace transforms of the coefficient functions lead to the spinor wave functions expressed as the Penrose transforms of the corresponding holomorphic functions on twistor space. We also consider the exponential generating function for the spinor wave functions and derive a novel representation for each of the spinor wave functions.

6 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
20222
2021547
2020529
2019519
2018525
2017572