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Impedance in
Accelerator Physics Accelerator physics is a branch of applied physics, concerned with designing, building and operating particle accelerators. As such, it can be described as the study of motion, manipulation and observation of relativistic charged particle beams ...
is a quantity that characterizes the self interaction of a charged particle beam, mediated by the beam environment, such as the
vacuum chamber A vacuum chamber is a rigid enclosure from which air and other gases are removed by a vacuum pump. This results in a low-pressure environment within the chamber, commonly referred to as a vacuum. A vacuum environment allows researchers to con ...
, RF cavities, and other elements encountered along the accelerator or
storage ring A storage ring is a type of circular particle accelerator in which a continuous or pulsed particle beam may be kept circulating typically for many hours. Storage of a particular particle depends upon the mass, momentum and usually the charge of t ...
.


Definition in terms of wakefunction

The impedance is defined as the Fourier transform of the Wakefunction. Z_0^(\omega) = \int_^\frace^W_0^'(z) From this expression and the fact that the wake function is real, one can derive the property: Z^(\omega) = Z^(-\omega)


Important sources of impedance

The impedance is defined at all positions along the beam trajectory. The beam travels through a
vacuum chamber A vacuum chamber is a rigid enclosure from which air and other gases are removed by a vacuum pump. This results in a low-pressure environment within the chamber, commonly referred to as a vacuum. A vacuum environment allows researchers to con ...
. Substantial impedance is generated in transitions, where the shape of the beam pipe changes. The RF cavities are another important source.


Impedance models

In the absence of detailed geometric modeling, one can use various models to represent different aspects of the accelerator beam pipe structure. One such model is the


Broadband resonator

For the longitudinal case, one has Z_(\omega) = R_s \frac with R_s the shunt impedance, Q, the quality factor, and \omega_r the resonant frequency.


Resistive Wall

Given a circular beam piper of radius b, and conductivity \sigma, the impedance is given by Z(\omega) = \frac\sqrt The corresponding longitudinal wakefield is approximately given by W(s) = \frac\sqrt\frac The transverse wake-function from the resistive wall is given by W(s) \approx \frac


Effect of Impedance on beam

The impedance acts back on the beam and can cause a variety of effects, often considered deleterious for accelerator functioning. In general, impedance effects are classified under the category of "collective effects" due to the fact that the whole beam must be considered together, and not just a single particle. The whole beam may, however, cause particular changes in the dynamics of individual particles such as tune shifts and coupling. Whole beam changes include emittance growth and instabilities that can lead to beam loss.


See also

https://impedance.web.cern.ch/impedance/


References

Accelerator physics {{accelerator-stub