Dominance of Radiation Pressure in Ion Acceleration with Linearly Polarized Pulses at Intensities of 1021 W cm-2
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Qiao, B.
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Queens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North Ireland
Univ Calif San Diego, Energy Res Ctr, La Jolla, CA 92093 USAQueens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North Ireland
Qiao, B.
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Kar, S.
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Queens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North IrelandQueens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North Ireland
Kar, S.
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Geissler, M.
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Queens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North IrelandQueens Univ Belfast, Sch Math & Phys, Belfast BT7 1NN, Antrim, North Ireland
A novel regime is proposed where, by employing linearly polarized laser pulses at intensities 10(21) W cm(-2) (2 orders of magnitude lower than discussed in previous work [T. Esirkepov et al., Phys. Rev. Lett. 92, 175003 (2004)]), ions are dominantly accelerated from ultrathin foils by the radiation pressure and have monoenergetic spectra. In this regime, ions accelerated from the hole-boring process quickly catch up with the ions accelerated by target normal sheath acceleration, and they then join in a single bunch, undergoing a hybrid light-sail-target normal sheath acceleration. Under an appropriate coupling condition between foil thickness, laser intensity, and pulse duration, laser radiation pressure can be dominant in this hybrid acceleration. Two-dimensional particle-in-cell simulations show that 1.26 GeV quasimonoenergetic C6+ beams are obtained by linearly polarized laser pulses at intensities of 10(21) W cm(-2).