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| 001 | 11463 | ||
| 005 | 20210129210543.0 | ||
| 024 | 7 | _ | |2 DOI |a 10.1103/PhysRevLett.105.155002 |
| 024 | 7 | _ | |2 WOS |a WOS:000282426400012 |
| 024 | 7 | _ | |2 Handle |a 2128/7254 |
| 037 | _ | _ | |a PreJuSER-11463 |
| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 550 |
| 084 | _ | _ | |2 WoS |a Physics, Multidisciplinary |
| 100 | 1 | _ | |0 P:(DE-Juel1)VDB90914 |a Qiao, B. |b 0 |u FZJ |
| 245 | _ | _ | |a Radiation-Pressure Acceleration of Ion Beams from Nanofoil Targets: The Leaky Light-Sail Regime |
| 260 | _ | _ | |a College Park, Md. |b APS |c 2010 |
| 300 | _ | _ | |a 155002 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a Output Types/Journal article |2 DataCite |
| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 336 | 7 | _ | |a ARTICLE |2 BibTeX |
| 336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
| 336 | 7 | _ | |a article |2 DRIVER |
| 440 | _ | 0 | |0 4925 |a Physical Review Letters |v 105 |x 0031-9007 |y 15 |
| 500 | _ | _ | |a B. Q. acknowledges the support from the Alexander von Humboldt Foundation. M. Z. thanks the support from the Royal Society. The work was also supported by EPSRC (Grants No. EP/C003586/1 and No. EP/D/06337X/1). Computing resources on JUROPA at JSC (Grants No. jzam04 and No. jjsc04) and VIP at RZG (collaboration grant with MPQ) are both acknowledged. |
| 520 | _ | _ | |a A new ion radiation-pressure acceleration regime, the "leaky light sail," is proposed which uses sub-skin-depth nanometer foils irradiated by circularly polarized laser pulses. In the regime, the foil is partially transparent, continuously leaking electrons out along with the transmitted laser field. This feature can be exploited by a multispecies nanofoil configuration to stabilize the acceleration of the light ion component, supplementing the latter with an excess of electrons leaked from those associated with the heavy ions to avoid Coulomb explosion. It is shown by 2D particle-in-cell simulations that a monoenergetic proton beam with energy 18 MeV is produced by circularly polarized lasers at intensities of just 10(19) W/cm(2). 100 MeV proton beams are obtained by increasing the intensities to 2 x 10(20) W/cm(2). |
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| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Zepf, M. |b 1 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Borghesi, M. |b 2 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Dromey, B. |b 3 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Geissler, M. |b 4 |
| 700 | 1 | _ | |0 P:(DE-Juel1)132156 |a Karmakar, A. |b 5 |u FZJ |
| 700 | 1 | _ | |0 P:(DE-Juel1)132115 |a Gibbon, P. |b 6 |u FZJ |
| 773 | _ | _ | |0 PERI:(DE-600)1472655-5 |a 10.1103/PhysRevLett.105.155002 |g Vol. 105, p. 155002 |p 155002 |q 105<155002 |t Physical review letters |v 105 |x 0031-9007 |y 2010 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1103/PhysRevLett.105.155002 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/11463/files/FZJ-11463.pdf |y OpenAccess |z Published final document. |
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| 914 | 1 | _ | |y 2010 |
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