Burst mode MHz repetition rate inverse free electron laser acceleration

The capability of accelerating electron bunches at high repetition rate is one of the key performance criteria for all high average power particle accelerator applications. High gradient laser-driven acceleration holds the potential for greatly reducing size and costs of future machines, but typical...

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Main Authors: N. Sudar, P. Musumeci, A. Ovodenko, A. Murokh, M. Polyanskiy, I. Pogorelsky, M. Fedurin, C. Swinson, K. Kusche, M. Babzien, M. Palmer
Format: Article
Language:English
Published: American Physical Society 2020-05-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.23.051301
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spelling doaj-0de0ce7ccd5844b89937ac8ef41fa5302020-11-25T02:10:34ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882020-05-0123505130110.1103/PhysRevAccelBeams.23.051301Burst mode MHz repetition rate inverse free electron laser accelerationN. SudarP. MusumeciA. OvodenkoA. MurokhM. PolyanskiyI. PogorelskyM. FedurinC. SwinsonK. KuscheM. BabzienM. PalmerThe capability of accelerating electron bunches at high repetition rate is one of the key performance criteria for all high average power particle accelerator applications. High gradient laser-driven acceleration holds the potential for greatly reducing size and costs of future machines, but typically requires very high peak laser powers. On the other hand, MHz pulse trains of TW-class laser beams are much beyond the state of the art, so that laser recycling and recirculation is a necessary step to bridge that gap. In this experiment we demonstrate for the first time an inverse free electron laser accelerator (IFEL) operating within an active optical cavity showing the ability to laser-accelerate electron bunch trains in burst mode at >20  MHz repetition rate. The experimental setup, synchronization challenges and acceleration results are presented. It is found that careful control of the dispersive properties of the cavity is required in order to sustain high accelerating gradients over many passes in the laser pulse train.http://doi.org/10.1103/PhysRevAccelBeams.23.051301
collection DOAJ
language English
format Article
sources DOAJ
author N. Sudar
P. Musumeci
A. Ovodenko
A. Murokh
M. Polyanskiy
I. Pogorelsky
M. Fedurin
C. Swinson
K. Kusche
M. Babzien
M. Palmer
spellingShingle N. Sudar
P. Musumeci
A. Ovodenko
A. Murokh
M. Polyanskiy
I. Pogorelsky
M. Fedurin
C. Swinson
K. Kusche
M. Babzien
M. Palmer
Burst mode MHz repetition rate inverse free electron laser acceleration
Physical Review Accelerators and Beams
author_facet N. Sudar
P. Musumeci
A. Ovodenko
A. Murokh
M. Polyanskiy
I. Pogorelsky
M. Fedurin
C. Swinson
K. Kusche
M. Babzien
M. Palmer
author_sort N. Sudar
title Burst mode MHz repetition rate inverse free electron laser acceleration
title_short Burst mode MHz repetition rate inverse free electron laser acceleration
title_full Burst mode MHz repetition rate inverse free electron laser acceleration
title_fullStr Burst mode MHz repetition rate inverse free electron laser acceleration
title_full_unstemmed Burst mode MHz repetition rate inverse free electron laser acceleration
title_sort burst mode mhz repetition rate inverse free electron laser acceleration
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2020-05-01
description The capability of accelerating electron bunches at high repetition rate is one of the key performance criteria for all high average power particle accelerator applications. High gradient laser-driven acceleration holds the potential for greatly reducing size and costs of future machines, but typically requires very high peak laser powers. On the other hand, MHz pulse trains of TW-class laser beams are much beyond the state of the art, so that laser recycling and recirculation is a necessary step to bridge that gap. In this experiment we demonstrate for the first time an inverse free electron laser accelerator (IFEL) operating within an active optical cavity showing the ability to laser-accelerate electron bunch trains in burst mode at >20  MHz repetition rate. The experimental setup, synchronization challenges and acceleration results are presented. It is found that careful control of the dispersive properties of the cavity is required in order to sustain high accelerating gradients over many passes in the laser pulse train.
url http://doi.org/10.1103/PhysRevAccelBeams.23.051301
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