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017 | _ | _ | |a This version is available at the following Publisher URL: http://apl.aip.org |
024 | 7 | _ | |a 10.1063/1.2200761 |2 DOI |
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024 | 7 | _ | |a 2128/2236 |2 Handle |
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082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Applied |
100 | 1 | _ | |a Anand, M. |b 0 |0 P:(DE-HGF)0 |
245 | _ | _ | |a Enhanced hard x-ray emission from microdroplet preplasma |
260 | _ | _ | |a Melville, NY |b American Institute of Physics |c 2006 |
300 | _ | _ | |a 181111 |
336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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440 | _ | 0 | |a Applied Physics Letters |x 0003-6951 |0 562 |v 88 |
500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
520 | _ | _ | |a We perform a comparative study of hard x-ray emission from femtosecond laser plasmas in 15 mu m methanol microdroplets and Perspex target. The hard x-ray yield from droplet plasmas is similar or equal to 68 times more than that obtained from solid plasmas at 2x10(15) W cm(-2). A 10 ns prepulse at about 5% of the main pulse appears to be essential for hard x-ray generation from droplets. Hot electron temperature of 36 keV is measured from the droplets at 8x10(14) W cm(-2), whereas a three times higher intensity is needed to obtain similar hot electron temperatures from Perspex plasmas. Particle-in-cell simulations with very long scale-length density profiles support experimental observations. (c) 2006 American Institute of Physics. |
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700 | 1 | _ | |a Kahaly, S. |b 1 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Ravindra Kumar, G. |b 2 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Krishnamurthy, M. |b 3 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Sandhu, A. S. |b 4 |0 P:(DE-HGF)0 |
700 | 1 | _ | |a Gibbon, P. |b 5 |u FZJ |0 P:(DE-Juel1)132115 |
773 | _ | _ | |a 10.1063/1.2200761 |g Vol. 88, p. 181111 |p 181111 |q 88<181111 |0 PERI:(DE-600)1469436-0 |t Applied physics letters |v 88 |y 2006 |x 0003-6951 |
856 | 7 | _ | |u http://dx.doi.org/10.1063/1.2200761 |u http://hdl.handle.net/2128/2236 |
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