Converting conventional electron accelerators to high peak brilliance Compton light sources

Several proposals have been put forward for converting electron accelerators to inverse Compton scattering (ICS) gamma sources. Typical approaches suggest combining near-IR solid-state lasers operating continuously at a multimegahertz repetition rate with e-beams when setting their interaction point...

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Main Authors: I. V. Pogorelsky, M. Polyanskiy, T. Shaftan
Format: Article
Language:English
Published: American Physical Society 2020-12-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.23.120702
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spelling doaj-2955f42c37c7411888e3cb9c761e05402021-02-11T23:55:03ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882020-12-01231212070210.1103/PhysRevAccelBeams.23.120702Converting conventional electron accelerators to high peak brilliance Compton light sourcesI. V. PogorelskyM. PolyanskiyT. ShaftanSeveral proposals have been put forward for converting electron accelerators to inverse Compton scattering (ICS) gamma sources. Typical approaches suggest combining near-IR solid-state lasers operating continuously at a multimegahertz repetition rate with e-beams when setting their interaction point inside a field-enhancement, Fabry-Perot optical cavity. We introduce here an alternative method of pairing particle accelerator beams with trains of long-wave-infrared, λ_{L}≈9–11  μm pulses from a picosecond CO_{2} laser of a novel architecture operating in a repetitive pulse-burst mode. Because of a considerable increase in the laser energy per pulse, combined with an order-of-magnitude higher number of laser photons per joule of laser energy, our approach allows us to increase the ICS peak flux and brilliance by 4 orders of magnitude compared to previous proposals while maintaining high (10^{11}–10^{12}  ph/s) average flux. This outcome is supported by the examples of the DAΦNE and CBETA accelerator facilities, where 10^{20}–10^{21}  ph/(s·mm^{2}·mrad^{2}·0.1%BW) peak brilliances at 50–1000 keV photon energy range can be achieved and is comparable or exceeds the capabilities of contemporary synchrotron light sources at hard x rays. Such high-brightness ICS sources will find applications in pump-probe and other ultrafast studies that require building up meaningful datasets on a single x-ray pulse.http://doi.org/10.1103/PhysRevAccelBeams.23.120702
collection DOAJ
language English
format Article
sources DOAJ
author I. V. Pogorelsky
M. Polyanskiy
T. Shaftan
spellingShingle I. V. Pogorelsky
M. Polyanskiy
T. Shaftan
Converting conventional electron accelerators to high peak brilliance Compton light sources
Physical Review Accelerators and Beams
author_facet I. V. Pogorelsky
M. Polyanskiy
T. Shaftan
author_sort I. V. Pogorelsky
title Converting conventional electron accelerators to high peak brilliance Compton light sources
title_short Converting conventional electron accelerators to high peak brilliance Compton light sources
title_full Converting conventional electron accelerators to high peak brilliance Compton light sources
title_fullStr Converting conventional electron accelerators to high peak brilliance Compton light sources
title_full_unstemmed Converting conventional electron accelerators to high peak brilliance Compton light sources
title_sort converting conventional electron accelerators to high peak brilliance compton light sources
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2020-12-01
description Several proposals have been put forward for converting electron accelerators to inverse Compton scattering (ICS) gamma sources. Typical approaches suggest combining near-IR solid-state lasers operating continuously at a multimegahertz repetition rate with e-beams when setting their interaction point inside a field-enhancement, Fabry-Perot optical cavity. We introduce here an alternative method of pairing particle accelerator beams with trains of long-wave-infrared, λ_{L}≈9–11  μm pulses from a picosecond CO_{2} laser of a novel architecture operating in a repetitive pulse-burst mode. Because of a considerable increase in the laser energy per pulse, combined with an order-of-magnitude higher number of laser photons per joule of laser energy, our approach allows us to increase the ICS peak flux and brilliance by 4 orders of magnitude compared to previous proposals while maintaining high (10^{11}–10^{12}  ph/s) average flux. This outcome is supported by the examples of the DAΦNE and CBETA accelerator facilities, where 10^{20}–10^{21}  ph/(s·mm^{2}·mrad^{2}·0.1%BW) peak brilliances at 50–1000 keV photon energy range can be achieved and is comparable or exceeds the capabilities of contemporary synchrotron light sources at hard x rays. Such high-brightness ICS sources will find applications in pump-probe and other ultrafast studies that require building up meaningful datasets on a single x-ray pulse.
url http://doi.org/10.1103/PhysRevAccelBeams.23.120702
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