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Inner Lindblad resonance in galaxies Nonlinear theory III The response density

For pt.II see ibid., vol.61, no.4, p.477 (1977). The authors calculate theoretically the response of a galaxy to an imposed spiral field. The unperturbed (axisymmetric) distribution function, f, changes considerably near the inner Lindblad resonance; the final distribution function, f/sub fin/, is f...

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Autor principal: Contopoulos, George
Lenguaje:eng
Publicado: 1979
Materias:
Acceso en línea:http://cds.cern.ch/record/875402
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author Contopoulos, George
author_facet Contopoulos, George
author_sort Contopoulos, George
collection CERN
description For pt.II see ibid., vol.61, no.4, p.477 (1977). The authors calculate theoretically the response of a galaxy to an imposed spiral field. The unperturbed (axisymmetric) distribution function, f, changes considerably near the inner Lindblad resonance; the final distribution function, f/sub fin/, is found by expressing f in terms of the 'resonant' integrals of motion and the corresponding angles, and averaging over the angles. Outside resonance the final distribution function is composed of three parts, two of them corresponding to trapped orbits, and one to untrapped orbits. The density response is found by integrating f/sub fin/ over all velocities. Away from the resonance the response can be expressed analytically. The physical meaning of the various terms of the response is discussed. Very near resonance the amplitude of the response is very large. The author also follows the azimuth of the response maximum going through the resonance. (11 refs).
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-8754022019-09-30T06:29:59Zhttp://cds.cern.ch/record/875402engContopoulos, GeorgeInner Lindblad resonance in galaxies Nonlinear theory III The response densityAstrophysics and AstronomyFor pt.II see ibid., vol.61, no.4, p.477 (1977). The authors calculate theoretically the response of a galaxy to an imposed spiral field. The unperturbed (axisymmetric) distribution function, f, changes considerably near the inner Lindblad resonance; the final distribution function, f/sub fin/, is found by expressing f in terms of the 'resonant' integrals of motion and the corresponding angles, and averaging over the angles. Outside resonance the final distribution function is composed of three parts, two of them corresponding to trapped orbits, and one to untrapped orbits. The density response is found by integrating f/sub fin/ over all velocities. Away from the resonance the response can be expressed analytically. The physical meaning of the various terms of the response is discussed. Very near resonance the amplitude of the response is very large. The author also follows the azimuth of the response maximum going through the resonance. (11 refs).oai:cds.cern.ch:8754021979
spellingShingle Astrophysics and Astronomy
Contopoulos, George
Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title_full Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title_fullStr Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title_full_unstemmed Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title_short Inner Lindblad resonance in galaxies Nonlinear theory III The response density
title_sort inner lindblad resonance in galaxies nonlinear theory iii the response density
topic Astrophysics and Astronomy
url http://cds.cern.ch/record/875402
work_keys_str_mv AT contopoulosgeorge innerlindbladresonanceingalaxiesnonlineartheoryiiitheresponsedensity