1990
DOI: 10.1016/0168-9002(90)91191-d
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Initial results of operating the rocketdyne undulator in a tapered configuration

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Cited by 13 publications
(6 citation statements)
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“…To deal with the high optical cavity power a group has proposed using an initial low power oscillator to bunch the beam which then provides high gain and extraction in a second wiggler [57]. Such a concept differs from earlier work on a MOPA (Master Oscillator Power Amplifier) [111] in that the electron transport to the second wiggler must maintain the electrons' phase coherence to the optical wavelength accuracy and so be of exceptionally high quality.…”
Section: Miscellaneous Approachesmentioning
confidence: 99%
“…To deal with the high optical cavity power a group has proposed using an initial low power oscillator to bunch the beam which then provides high gain and extraction in a second wiggler [57]. Such a concept differs from earlier work on a MOPA (Master Oscillator Power Amplifier) [111] in that the electron transport to the second wiggler must maintain the electrons' phase coherence to the optical wavelength accuracy and so be of exceptionally high quality.…”
Section: Miscellaneous Approachesmentioning
confidence: 99%
“…Superconducting energy recovery linacs are the primary drivers for high average power FEL oscillators [64][65][66][67][68][69][70]; however, other types of FEL oscillators have used various techniques to increase the output pulse energy including, but not limited to, optical klystrons [34,36,48,57,58,60,63,[71][72][73][74][75][76], cavity dumping [77][78][79][80][81], pulse stacking in an external cavity [82][83][84], electron beam energy ramping [85,86] or dynamic cavity desynchronization [87][88][89][90][91][92]. Tapering of the undulator [93][94][95] has also been used to improve the peak power in the pulse [96][97][98][99][100], however, tapering of the undulator in FEL oscillators leads to complicated dynamics and a strong dependence on system parameters [101]…”
Section: Introductionmentioning
confidence: 99%
“…Operation at other wavelength ranges is possible through harmonic generation [105][106][107] and such harmonics were quickly observed [40]. Lasing on the third harmonic was first demonstrated using the Standford MARK-III FEL oscillator [108], quickly followed by others [43,48,58,61,97,[109][110][111][112][113][114][115][116][117][118][119][120][121]. The simultaneous generation of multiple wavelengths may be beneficial for certain applications.…”
Section: Introductionmentioning
confidence: 99%
“…Superconducting energy-recovery linacs are the primary drivers for high average power FEL oscillators [63][64][65][66][67][68][69]; however, other types of FEL oscillators have used various techniques to increase the output pulse energy including but not limited to optical klystrons [33,35,47,56,57,59,62,[70][71][72][73][74][75], cavity dumping [76][77][78][79][80], pulse stacking in an external cavity [81][82][83], electron beam energy ramping [84,85] or dynamic cavity desynchronization [86][87][88][89][90][91]. Tapering of the undulator has also been used to improve the peak power in the pulse [92][93][94][95][96], however, tapering of the undulator in FEL oscillators leads to complicated dynamics and strong dependence on system parameters [97][98][99][100].…”
Section: Introductionmentioning
confidence: 99%