2009
DOI: 10.1103/physrevstab.12.033501
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Theoretical and experimental study of passive spatiotemporal shaping of picosecond laser pulses

Abstract: We report the results of theoretical and experimental studies on passive spatiotemporal shaping of cw mode-locked picosecond laser pulses for driving the photocathode of a high-brightness, high-current energy recovery linear accelerator. The temporal pulse shape is modified using birefringent crystals, while a refractive optical system is used to generate a flattop spatial beam profile. An optical transport system is designed and implemented to deliver the flattop pulse onto a photocathode sited 9 m away from … Show more

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Cited by 35 publications
(23 citation statements)
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“…The development of the necessary spatial and temporal shaping techniques is an ongoing project: proof-of-principle experiments have been successfully carried out with a laser of similar pulse width, operating at 532 nm and 81.5 MHz. A transport line has been designed and built and the propagation of a shaped pulse through it to the photocathode simulated and tested experimentally [4]. As the performance of the complete photocathode drive system is critical for ERL operation, an extensive set of diagnostics will be in place to monitor and maintain its performance.…”
Section: Laser Systemmentioning
confidence: 99%
“…The development of the necessary spatial and temporal shaping techniques is an ongoing project: proof-of-principle experiments have been successfully carried out with a laser of similar pulse width, operating at 532 nm and 81.5 MHz. A transport line has been designed and built and the propagation of a shaped pulse through it to the photocathode simulated and tested experimentally [4]. As the performance of the complete photocathode drive system is critical for ERL operation, an extensive set of diagnostics will be in place to monitor and maintain its performance.…”
Section: Laser Systemmentioning
confidence: 99%
“…There are two approaches to doing this. One method is to use a number N of birefringent crystals to progressively duplicate and timeshift pulses such that the resulting series of 2 N pulses overlap in such a way as to sum to a flat top pulse [2][3][4]. This technique is illustrated for an eight-pulse series in Fig.…”
Section: Temporal Shapingmentioning
confidence: 99%
“…Further experimental details can be found in Ref. [4] Static phase differences between replicas can arise from unequal path lengths traversed by the ordinary and extraordinary pulses, as a result of the tilt of the crystal plane. These phase differences can change over time due to thermal expansion and temperaturedependent birefringence of the crystals, particularly since the optical absorption in this case is significant (32% over all 3 crystals).…”
Section: Temporal Shapingmentioning
confidence: 99%
“…This shaper worked very well when supplied with a good quality Gaussian beam with a precise initial size and divergence, but it was not realistic to use this in practice with our nonideal input beam, and more importantly it does not allow for a tunable shape. See also [19]. Similarly, we also tested an engineered diffuser (Thorlabs ED1-C20) which produces a uniform flattop speckle pattern for an arbitrary input beam.…”
Section: Introductionmentioning
confidence: 99%