2004
DOI: 10.1016/j.nima.2004.04.040
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Consideration on the BPM alignment tolerance in X-ray FELs

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Cited by 30 publications
(54 citation statements)
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“…If the electron moves along a trajectory deviated from a straight line, the FEL gain is significantly reduced because of the mechanisms explained in [3,4].…”
Section: A Trajectory Errormentioning
confidence: 99%
See 1 more Smart Citation
“…If the electron moves along a trajectory deviated from a straight line, the FEL gain is significantly reduced because of the mechanisms explained in [3,4].…”
Section: A Trajectory Errormentioning
confidence: 99%
“…The latter is in principle corrected by steering the electron beam so that it goes through the origins of beam position monitors (BPMs) that are aligned in line. It should be noted, however, that the alignment accuracy of BPMs with a conventional survey method is usually insufficient to achieve lasing, especially in the angstrom-wavelength region because the tolerance of the trajectory straightness becomes more stringent for shorter wavelengths [4].…”
Section: A Trajectory Errormentioning
confidence: 99%
“…Because the overlap between them determines the strength of nonlinear interaction in order to form electron microbunches. Single-kick errors [6] due to position misalignments of the accelerator components decrease OF. For example, these misalignments are caused by position differences among the magnetic centers of quadrupole magnets and the error dipole field of the undulators.…”
Section: Introductionmentioning
confidence: 99%
“…Ref. [1] states that the gain degradation mainly comes from single kick errors (SKE) caused by mis-aligned quadrupole magnets, and error dipole fields of the undulators. To reduce the gain degradation, the angle of SKE should be well below a critical angle, y c , which is defined…”
Section: Introductionmentioning
confidence: 99%
“…In the case of the x-ray free-electron laser (XFEL) facility SACLA (SPring-8 Angstrom Compact free-electron LAser) [2], for example, consisting of a 8-GeV linear accelerator and a 100 mlong undulator beamline, y c at a wavelength of 0.1 nm is approximately 5 mrad [1]. Since the interval of BPMs is approximately 6 m in the undulator section, the beam position should be controlled within much less than 30 mm from a straight line.…”
Section: Introductionmentioning
confidence: 99%