TY - JOUR
T1 - Gamma-rays from harmonically resonant betatron oscillations in a plasma wake
AU - Cipiccia, Silvia
AU - Islam, Mohammad
AU - Ersfeld, Bernhard
AU - Shanks, Richard
AU - Brunetti, Enrico
AU - Vieux, Gregory
AU - Yang, Xue
AU - Issac, Riju
AU - Wiggins, Samuel
AU - Welsh, Gregor
AU - Anania, Maria Pia
AU - Maneuski, Dzmitry
AU - Montgomery, Rachel
AU - Smith, Gary
AU - Hoek, Matthias
AU - Hamilton, David J.
AU - Lemos, Nuno R. C.
AU - Symes, Dan
AU - Rajeev, Pattathil P.
AU - Shea, Val O.
AU - Dias, João M.
AU - Jaroszynski, Dino A.
PY - 2011/9/18
Y1 - 2011/9/18
N2 - An intense laser pulse in a plasma can accelerate electrons1, 2, 3, 4 to GeV energies in centimetres5, 6, 7. Transverse betatron motion8, 9 in the plasma wake results in X-ray photons with an energy that depends on the electron energy, oscillation amplitude and frequency of the betatron motion10, 11, 12. Betatron X-rays from laser-accelerator electrons have hitherto been limited to spectra peaking between 1 and 10 keV (ref. 13). Here we show that the betatron amplitude is resonantly enhanced when electrons interact with the rear of the laser pulse14, 15. At high electron energy, resonance occurs when the laser frequency is a harmonic of the betatron frequency, leading to a significant increase in the photon energy. 108 gamma-ray photons, with spectra peaking between 20 and 150 keV, and a peak brilliance >1023 photons s−1 mrad−2 mm−2 per 0.1% bandwidth, are measured for 700 MeV beams, with 107 photons emitted between 1 and 7 MeV. Femtosecond duration gamma-rays may find uses in imaging, isotope production, probing dense matter, homeland security and nuclear physics16.
AB - An intense laser pulse in a plasma can accelerate electrons1, 2, 3, 4 to GeV energies in centimetres5, 6, 7. Transverse betatron motion8, 9 in the plasma wake results in X-ray photons with an energy that depends on the electron energy, oscillation amplitude and frequency of the betatron motion10, 11, 12. Betatron X-rays from laser-accelerator electrons have hitherto been limited to spectra peaking between 1 and 10 keV (ref. 13). Here we show that the betatron amplitude is resonantly enhanced when electrons interact with the rear of the laser pulse14, 15. At high electron energy, resonance occurs when the laser frequency is a harmonic of the betatron frequency, leading to a significant increase in the photon energy. 108 gamma-ray photons, with spectra peaking between 20 and 150 keV, and a peak brilliance >1023 photons s−1 mrad−2 mm−2 per 0.1% bandwidth, are measured for 700 MeV beams, with 107 photons emitted between 1 and 7 MeV. Femtosecond duration gamma-rays may find uses in imaging, isotope production, probing dense matter, homeland security and nuclear physics16.
KW - wakefield accelerators
KW - betatron oscillations
KW - plasma wakes
UR - http://www.scopus.com/inward/record.url?scp=80555150655&partnerID=8YFLogxK
U2 - 10.1038/nphys2090
DO - 10.1038/nphys2090
M3 - Letter
SN - 1745-2473
VL - 7
SP - 867
EP - 871
JO - Nature Physics
JF - Nature Physics
ER -