Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Radiation and Scattering Processes

Sune R. Svanberg

Published Jan 1, 1991• 0 citations
Publisher
DOI
10.1007/978-3-642-97258-4_4

Related papers

Radiation and Scattering Processes

Sune R. Svanberg

Advanced texts in physics•Jan 1, 2004•0 citations

Radiation and Scattering Processes

Sune R. Svanberg

Springer series on atomic, optical, and plasma physics•Jan 1, 2001•0 citations

Radiation and Scattering Processes

Sune R. Svanberg

Graduate texts in physics•Jan 1, 2022•0 citations

Radiation and Scattering Processes

Sune R. Svanberg

Springer eBooks•Jan 1, 1992•0 citations

Stimulated scattering of nonmonochromatic radiation

Igor' M Bel'dyugin, E M Zemskov

A theoretical study is made of the stimulated scattering of radiation whose spectrum is much wider than the frequency of a vibrational transition in the scattering medium. It is shown that the efficiency of the scattering process then depends strongly on the statistical properties of the incident (pump) radiation.

Soviet Journal of Quantum Electronics•Jan 31, 1980•7 citations

Incoherent properties of induced radiation

B. A. Veklenko

The evolution of a quantized electromagnetic field in a thermally excited dispersion medium is determined by two scattering channels. The coherent channel is formed exclusively by the elastic scattering of quanta. The incoherent channel, along with elastic scattering processes, necessarily contains inelastic scattering processes, including induced radiation. Interference between the channels is absent because of the orthogonality of the wave functions of the medium in its final states, which correspond to different scattering channels. Therefore, in an excited medium, interference processes that are not described by its refractive index may arise. An interference pattern of this kind can be formed, in particular, as a result of the superposition of the resonance radiation incident on an excited medium and the radiation reflected from this medium. In this case, the conventional perturbation theory proves to be inadequate.

Optics and Spectroscopy•May 1, 2003•2 citations
The evolution of a quantized electromagnetic field in a thermally excited dispersion medium is determined by two scattering channels. The coherent channel is formed exclusively by the elastic scattering of quanta. The incoherent channel, along with elastic scattering processes, necessarily contains inelastic scattering processes, including induced radiation. Interference between the channels is absent because of the orthogonality of the wave functions of the medium in its final states, which correspond to different scattering channels. Therefore, in an excited medium, interference processes that are not described by its refractive index may arise. An interference pattern of this kind can be formed, in particular, as a result of the superposition of the resonance radiation incident on an excited medium and the radiation reflected from this medium. In this case, the conventional perturbation theory proves to be inadequate.