2015 40th International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz) 2015
DOI: 10.1109/irmmw-thz.2015.7327519
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Coherent radiation sources based on laser driven plasma waves

Abstract: Here we explore ways of converting laser radiation into coherent electromagnetic radiation using laser-driven plasma waves. Several schemes are presented, including colliding laser pulses in magnetized plasma and utilizing ultra-short electron bunches from laser wakefield accelerators to produce intense single-cycle pulses through coherent transition radiation and few-cycle coherent synchrotron radiation in undulators and plasma channels. These sources rely on high current electron bunches with femtosecond dur… Show more

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Cited by 3 publications
(2 citation statements)
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“…Electron beam energy spectra are measured using an imaging dipole magnet spectrometer and the beam is transported to an undulator using sets of quadrupole magnets. Beams with an emittance of 1 π mm mrad 17 , energies of 80-300 MeV 1,2,4,11 , and percent level energy spreads 2,4,18 , low divergences (0.5-2 mrad) 18 , peak currents >1 kA and fs bunch duration 5 have been measured on the ALPHA-X beamline ( Figure 2). Theoretical studies ( Figure 1) show that attosecond bunches can be produced by perturbing the plasma density to briefly trigger injection 6 .…”
Section: Lwfa Experimentsmentioning
confidence: 99%
“…Electron beam energy spectra are measured using an imaging dipole magnet spectrometer and the beam is transported to an undulator using sets of quadrupole magnets. Beams with an emittance of 1 π mm mrad 17 , energies of 80-300 MeV 1,2,4,11 , and percent level energy spreads 2,4,18 , low divergences (0.5-2 mrad) 18 , peak currents >1 kA and fs bunch duration 5 have been measured on the ALPHA-X beamline ( Figure 2). Theoretical studies ( Figure 1) show that attosecond bunches can be produced by perturbing the plasma density to briefly trigger injection 6 .…”
Section: Lwfa Experimentsmentioning
confidence: 99%
“…6 Only a small fraction of plasma electrons can be injected into the bubble and laser-wakefield accelerators typically produce beams with a small charge at pC level, which is desirable when high-quality beams with short bunch length, narrow energy spread and low emittance are required, for novel radiation sources. [7][8][9][10][11][12][13][14] There are, however, applications such as non-destructive-testing, ultra-fast studies in condensed matter, radiolysis, isotope production and radiotherapy that require high-charge, low-energy electron beams. [15][16][17][18][19] Ionization-assisted injection in high-Z or clustering gas targets has been explored to boost the charge to 100s pC at 10s-100s MeV energies.…”
Section: Introductionmentioning
confidence: 99%