Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range

A comprehensive analysis is presented that describes amplification of a seed THz pulse in a single-pass free-electron laser (FEL) driven by a photoinjector. The dynamics of the radiation pulse and the modulated electron beam are modeled using the time-dependent FEL code, GENESIS 1.3. A 10-ps (FWHM)...

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Main Authors: C. Sung, S. Ya. Tochitsky, S. Reiche, J. B. Rosenzweig, C. Pellegrini, C. Joshi
Format: Article
Language:English
Published: American Physical Society 2006-12-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.9.120703
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spelling doaj-3c2107dea1e44edb8b9743c2f3e486042020-11-24T21:26:29ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022006-12-0191212070310.1103/PhysRevSTAB.9.120703Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz rangeC. SungS. Ya. TochitskyS. ReicheJ. B. RosenzweigC. PellegriniC. JoshiA comprehensive analysis is presented that describes amplification of a seed THz pulse in a single-pass free-electron laser (FEL) driven by a photoinjector. The dynamics of the radiation pulse and the modulated electron beam are modeled using the time-dependent FEL code, GENESIS 1.3. A 10-ps (FWHM) electron beam with a peak current of 50–100 A allows amplification of a ∼1  kW seed pulse in the frequency range 0.5–3 THz up to 10–100 MW power in a relatively compact 2-m long planar undulator. The electron beam driving the FEL is strongly modulated, with some inhomogeneity due to the slippage effect. It is shown that THz microbunching of the electron beam is homogeneous over the entire electron pulse when saturated FEL amplification is utilized at the very entrance of an undulator. This requires seeding of a 30-cm long undulator buncher with a 1–3 MW of pump power with radiation at the resonant frequency. A narrow-band seed pulse in the THz range needed for these experiments can be generated by frequency mixing of CO_{2} laser lines in a GaAs nonlinear crystal. Two schemes for producing MW power pulses in seeded FELs are considered in some detail for the beam parameters achievable at the Neptune Laboratory at UCLA: the first uses a waveguide to transport radiation in the 0.5–3 THz range through a 2-m long FEL amplifier and the second employs high-gain third harmonic generation using the FEL process at 3–9 THz.http://doi.org/10.1103/PhysRevSTAB.9.120703
collection DOAJ
language English
format Article
sources DOAJ
author C. Sung
S. Ya. Tochitsky
S. Reiche
J. B. Rosenzweig
C. Pellegrini
C. Joshi
spellingShingle C. Sung
S. Ya. Tochitsky
S. Reiche
J. B. Rosenzweig
C. Pellegrini
C. Joshi
Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
Physical Review Special Topics. Accelerators and Beams
author_facet C. Sung
S. Ya. Tochitsky
S. Reiche
J. B. Rosenzweig
C. Pellegrini
C. Joshi
author_sort C. Sung
title Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
title_short Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
title_full Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
title_fullStr Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
title_full_unstemmed Seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
title_sort seeded free-electron and inverse free-electron laser techniques for radiation amplification and electron microbunching in the terahertz range
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2006-12-01
description A comprehensive analysis is presented that describes amplification of a seed THz pulse in a single-pass free-electron laser (FEL) driven by a photoinjector. The dynamics of the radiation pulse and the modulated electron beam are modeled using the time-dependent FEL code, GENESIS 1.3. A 10-ps (FWHM) electron beam with a peak current of 50–100 A allows amplification of a ∼1  kW seed pulse in the frequency range 0.5–3 THz up to 10–100 MW power in a relatively compact 2-m long planar undulator. The electron beam driving the FEL is strongly modulated, with some inhomogeneity due to the slippage effect. It is shown that THz microbunching of the electron beam is homogeneous over the entire electron pulse when saturated FEL amplification is utilized at the very entrance of an undulator. This requires seeding of a 30-cm long undulator buncher with a 1–3 MW of pump power with radiation at the resonant frequency. A narrow-band seed pulse in the THz range needed for these experiments can be generated by frequency mixing of CO_{2} laser lines in a GaAs nonlinear crystal. Two schemes for producing MW power pulses in seeded FELs are considered in some detail for the beam parameters achievable at the Neptune Laboratory at UCLA: the first uses a waveguide to transport radiation in the 0.5–3 THz range through a 2-m long FEL amplifier and the second employs high-gain third harmonic generation using the FEL process at 3–9 THz.
url http://doi.org/10.1103/PhysRevSTAB.9.120703
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