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Coupling impedances of small discontinuities: Dependence on beam velocity

Sergey S. Kurennoy
Phys. Rev. ST Accel. Beams 9, 054201 – Published 23 May 2006

Abstract

The beam coupling impedances of small discontinuities of an accelerator vacuum chamber have been calculated [e.g., Kurennoy, Gluckstern, and Stupakov, Phys. Rev. E 52, 4354 (1995)] for ultrarelativistic beams using the Bethe diffraction theory. Here we extend the results to an arbitrary beam velocity. The vacuum chamber is assumed to have an arbitrary, but uniform along the beam path, cross section. The longitudinal and transverse coupling impedances are derived in terms of series over cross-section eigenfunctions, while the discontinuity shape enters via its polarizabilities. Simple explicit formulas for two important particular cases—circular and rectangular chamber cross sections—are presented. The impedance dependence on the beam velocity exhibits some unusual features: for example, the reactive impedance, which dominates in the ultrarelativistic limit, can vanish at a certain beam velocity, or its magnitude can exceed the ultrarelativistic value many times. In addition, we demonstrate that the same technique, the field expansion into a series of cross-section eigenfunctions, is convenient for calculating the space-charge impedance of uniform beam pipes with arbitrary cross section.

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  • Received 22 March 2006

DOI:https://doi.org/10.1103/PhysRevSTAB.9.054201

This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Authors & Affiliations

Sergey S. Kurennoy

  • Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA

Article Text

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Issue

Vol. 9, Iss. 5 — May 2006

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Images

  • Figure 1
    Figure 1
    The ratio of the longitudinal impedance (29) to its relativistic value for a circular hole in a round pipe versus β=v/c for ωb/c=0.1,0.25,0.5,1 (solid, short-dashed, dashed, and long-dashed curves).Reuse & Permissions
  • Figure 2
    Figure 2
    The same, for a small semispherical protrusion.Reuse & Permissions
  • Figure 3
    Figure 3
    Direction φd of the transverse impedance (40) versus hole position on the side wall of a square chamber for ωb/(πβγc)=0,3,10 (short-dashed, dashed, and long-dashed curves). The solid line is for a circular pipe.Reuse & Permissions
  • Figure 4
    Figure 4
    Normalized magnitude of function d in Eq. (40) versus κb/π for three hole positions h=yh/b=0.5,0.75,0.9 on the side wall of a square chamber (short-dashed, dashed, and long-dashed curves). The solid line shows for comparison κb/2/I1(κb) from Eq. (39).Reuse & Permissions
  • Figure 5
    Figure 5
    Function S (45) for a square chamber versus the ratio ζ of the beam size to the chamber size a at three different values of w=κa/π=0,1,10 (short-dashed, dashed, and long-dashed curves). The solid curve shows the analytical relativistic limit ln(1/ζ)/(2π).Reuse & Permissions
  • Figure 6
    Figure 6
    The same versus w=κa/π for three different beam sizes ζa, ζ=0.001,0.01,0.1 (short-dashed, dashed, and long-dashed curves).Reuse & Permissions
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