Phys. Rev. ST Accel. Beams 6, 034206 (2003) [18 pages]Stochastic-hydrodynamic model of halo formation in charged particle beams |
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Nicola Cufaro Petroni *
Dipartimento Interateneo di Matematica, Università e Politecnico di Bari, T.I.R.E.S. (Innovative Technologies for Signal Detection and Processing), Università di Bari, Istituto Nazionale di Fisica Nucleare, Sezione di Bari, Istituto Nazionale per la Fisica della Materia, Unità di Bari, Via G. Amendola 173, 70126 Bari, Italy
Salvatore De Martino †, Silvio De Siena ‡, and Fabrizio Illuminati §
Dipartimento di Fisica “E. R. Caianiello,” Università di Salerno, Istituto Nazionale per la Fisica della Materia, Unità di Salerno, Istituto Nazionale di Fisica Nucleare, Sezione di Napoli (Gruppo collegato di Salerno), Via S. Allende, I-84081 Baronissi (SA), Italy
Received 30 December 2002; published 27 March 2003
The formation of the beam halo in charged particle accelerators is studied in the framework of a stochastic-hydrodynamic model for the collective motion of the particle beam. In such a stochastic-hydrodynamic theory the density and the phase of the charged beam obey a set of coupled nonlinear hydrodynamic equations with explicit time-reversal invariance. This leads to a linearized theory that describes the collective dynamics of the beam in terms of a classical Schrödinger equation. Taking into account space-charge effects, we derive a set of coupled nonlinear hydrodynamic equations. These equations define a collective dynamics of self-interacting systems much in the same spirit as in the Gross-Pitaevskii and Landau-Ginzburg theories of the collective dynamics for interacting quantum many-body systems. Self-consistent solutions of the dynamical equations lead to quasistationary beam configurations with enhanced transverse dispersion and transverse emittance growth. In the limit of a frozen space-charge core it is then possible to determine and study the properties of stationary, stable core-plus-halo beam distributions. In this scheme the possible reproduction of the halo after its elimination is a consequence of the stationarity of the transverse distribution which plays the role of an attractor for every other distribution.
©2003 The American Physical Society
URL: http://link.aps.org/abstract/PRSTAB/v6/e034206
DOI: 10.1103/PhysRevSTAB.6.034206
PACS: 02.50.Ey, 05.40.–a, 29.27.Bd, 41.85.Ew
* Electronic address: cufaro@ba.infn.it
† Electronic address: demartino@sa.infn.it
‡ Electronic address: desiena@sa.infn.it
§ Electronic address: illuminati@sa.infn.it
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