2002
DOI: 10.1103/physrevstab.5.064401
|View full text |Cite|
|
Sign up to set email alerts
|

Coherent synchrotron radiation instability in a bunch compressor

Abstract: The coherent synchrotron radiation of a bunch in a bunch compressor may lead to the microwave instability producing longitudinal modulation of the bunch with wavelengths small compared to the bunch length. It can also be a source of an undesirable emittance growth in the compressor. We derive and analyze the equation that describes linear evolution of the microwave modulation taking into account incoherent energy spread and finite emittance of the beam. Numerical solution of this equation for the Linac Coheren… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
77
0

Year Published

2003
2003
2023
2023

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 154 publications
(78 citation statements)
references
References 5 publications
1
77
0
Order By: Relevance
“…It is assumed here that energy modulations are accumulated upstream of the chicane but not inside: there the self-interaction is suppressed due to R 51 and R 52 effects [11][12][13]. We also assume in the following that a length of the drift space is much larger than that of the chicane, while the R 56 of the drift space is much smaller.…”
Section: B Formula For a Gain Per Cascadementioning
confidence: 99%
See 1 more Smart Citation
“…It is assumed here that energy modulations are accumulated upstream of the chicane but not inside: there the self-interaction is suppressed due to R 51 and R 52 effects [11][12][13]. We also assume in the following that a length of the drift space is much larger than that of the chicane, while the R 56 of the drift space is much smaller.…”
Section: B Formula For a Gain Per Cascadementioning
confidence: 99%
“…It is advisable to reduce it (if technically possible), since the wavelength (8) and length of the drift space (12) are also reduced but the gain (13) stays the same. This happens until the spread of longitudinal velocities starts playing a role, i.e.…”
Section: Formulas For An Optimized Lsc Amplifiermentioning
confidence: 99%
“…The effect of radiation shielding [21][22][23] is neglected, since the wavelength at which the CSR starts being suppressed by the vacuum chamber [22], ! 2hĂ°h=RÞ 1=2 ffi 1 mm (h is the vacuum chamber gap and R the bending radius), is much longer than the electron bunch length, 40 m z 80 m. Particle-field interactions on a scale much shorter than the bunch length such as those driving the so-called microbunching instability [24][25][26][27] are ignored on the ground that the analysis of the microbunching instability [26,27] predicts a small gain for the experimental configuration of this study. For the sake of simplicity, the CSR emission and its interaction with the electrons is described below within the bounds of the single-kick approximation.…”
mentioning
confidence: 94%
“…As a bunch propagates through the bends of a magnetic bunch compressor, the tail-head interaction due to CSR induces increased beam energy spread and transverse emittance dilution that can degrade the downstream FEL performance [1][2][3]. In addition, the CSR interaction is known to generate a microbunching instability in which large-amplitude current modulations can grow from small-amplitude, shortwavelength variations in the initial current profile [4,5].…”
Section: Introductionmentioning
confidence: 99%