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000020325 1001_ $$0P:(DE-HGF)0$$aQiao, B.$$b0
000020325 245__ $$aDominance of Radiation Pressure in Ion Acceleration with Linearly Polarized Pulses at Intensities of 1021  W cm-2
000020325 260__ $$aCollege Park, Md.$$bAPS$$c2012
000020325 300__ $$a115002
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000020325 440_0 $$04925$$aPhysical Review Letters$$v108$$x0031-9007$$y11
000020325 500__ $$aWe acknowledge helpful discussions with A. Macchi, J. Schreiber, and B. Dromey. The work is supported by EPSRC (Grants No. EP/E035728/1 and No. EP/D/06337X/1). Computing resources from e-Science facility of RAL-STFC are also acknowledged.
000020325 520__ $$aA novel regime is proposed where, by employing linearly polarized laser pulses at intensities 10(21) W cm(-2) (2 orders of magnitude lower than discussed in previous work [T. Esirkepov et al., Phys. Rev. Lett. 92, 175003 (2004)]), ions are dominantly accelerated from ultrathin foils by the radiation pressure and have monoenergetic spectra. In this regime, ions accelerated from the hole-boring process quickly catch up with the ions accelerated by target normal sheath acceleration, and they then join in a single bunch, undergoing a hybrid light-sail-target normal sheath acceleration. Under an appropriate coupling condition between foil thickness, laser intensity, and pulse duration, laser radiation pressure can be dominant in this hybrid acceleration. Two-dimensional particle-in-cell simulations show that 1.26 GeV quasimonoenergetic C6+ beams are obtained by linearly polarized laser pulses at intensities of 10(21) W cm(-2).
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000020325 7001_ $$0P:(DE-HGF)0$$aKar, S.$$b1
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000020325 8567_ $$uhttp://dx.doi.org/10.1103/PhysRevLett.108.115002
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