Enhanced laser wakefield acceleration using dual-color relativistic pulses
In a recent article by Liet al(2019Sci. Adv.5. eaav7940), experimental results from a dual-color laser wakefield acceleration (LWFA) were presented. In the present paper we, primarily, focus on detailed simulation studies of such a scheme in the self-injection and ionization injection regimes, respe...
Elmentve itt :
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| Dokumentumtípus: | Cikk |
| Megjelent: |
2020
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| Sorozat: | PLASMA PHYSICS AND CONTROLLED FUSION
62 No. 9 |
| Tárgyszavak: | |
| doi: | 10.1088/1361-6587/aba481 |
| mtmt: | 31774573 |
| Online Access: | http://publicatio.bibl.u-szeged.hu/26942 |
| LEADER | 02633nab a2200313 i 4500 | ||
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| 008 | 230406s2020 hu o 0|| Angol d | ||
| 022 | |a 0741-3335 | ||
| 024 | 7 | |a 10.1088/1361-6587/aba481 |2 doi | |
| 024 | 7 | |a 31774573 |2 mtmt | |
| 040 | |a SZTE Publicatio Repozitórium |b hun | ||
| 041 | |a Angol | ||
| 100 | 1 | |a Hafiz Nasr Abdelrahman Mohamed | |
| 245 | 1 | 0 | |a Enhanced laser wakefield acceleration using dual-color relativistic pulses |h [elektronikus dokumentum] / |c Hafiz Nasr Abdelrahman Mohamed |
| 260 | |c 2020 | ||
| 300 | |a 13 | ||
| 490 | 0 | |a PLASMA PHYSICS AND CONTROLLED FUSION |v 62 No. 9 | |
| 520 | 3 | |a In a recent article by Liet al(2019Sci. Adv.5. eaav7940), experimental results from a dual-color laser wakefield acceleration (LWFA) were presented. In the present paper we, primarily, focus on detailed simulation studies of such a scheme in the self-injection and ionization injection regimes, respectively. The spatiotemporally-overlapped 30 fs dual-color laser pulses are at fundamental (FL, 800 nm, 'red') and second-harmonic (SH, 400 nm, 'blue') wavelengths. They are (a) co-propagating in an under-dense plasma, (b) relativistically intense (I> 10(18)W cm(-2)) and (c) having relatively high-energy (multi-Joule, loose focusing) and low-energy (sub-Joule, tight focusing), respectively. The basic concept of the scheme is the fact that the depletion length (L-pd) for a relativistic laser pulse in an under-dense plasma has an inverse quadratic dependence on the laser wavelength (proportional to 1/lambda(2)). Here, first by using a single FL 77 TW/30 fs laser pulse to drive a LWFA, an electron beam was accelerated up to similar to 400 MeV from a background plasma having an electron density of 10(19)cm(-3). Then, by driving the same LWFA by co-propagating 'blue' 7 TW/30 fs and 'red' 70 TW/30 fs laser pulses, the electron energy reached similar to 700-800 MeV (maximum). The simulations confirm that in such a dual-color LWFA scheme, the role of the SH laser pulse is post-accelerating electrons after a rapid depletion of the FL laser pulse in the plasma. Furthermore, the SH pulse assists the ionization-injection of the electrons which is an additional benefit of the dual-color LWFA scheme. | |
| 650 | 4 | |a Fizikai tudományok | |
| 700 | 0 | 1 | |a Li Guangyu |e aut |
| 700 | 0 | 1 | |a Li Song |e aut |
| 700 | 0 | 1 | |a Ain Quratul |e aut |
| 700 | 0 | 1 | |a Gao Kai |e aut |
| 700 | 0 | 1 | |a Saeed Muhammad |e aut |
| 700 | 0 | 1 | |a Papp Dániel |e aut |
| 700 | 0 | 1 | |a Zhu Jianqiang |e aut |
| 700 | 0 | 1 | |a Kamperidis Christos |e aut |
| 856 | 4 | 0 | |u http://publicatio.bibl.u-szeged.hu/26942/1/31774573.pdf |z Dokumentum-elérés |