Enhanced laser wakefield acceleration using dual-color relativistic pulses. (30th July 2020)

• Record Type: Journal Article
• Authors: Hafz, Nasr A M; Li, Guangyu; Li, Song; Ain, Quratul; Gao, Kai; Saeed, Muhammad; Papp, Daniel; Zhu, Jianqiang; Kamperidis, Christos
• Is Part Of: Plasma physics and controlled fusion. Volume 62:Number 9(2020)
• Publication Date: 2020-07-30
• Subjects: dual-color laser-plasma accelerator -- laser wakefield acceleration -- self-injection -- ionization injection -- PIC simulation; Plasma (Ionized gases) -- Periodicals; Controlled fusion -- Periodicals; 530.44
• DOI: 10.1088/1361-6587/aba481
• Languages: English
• ISSNs: 0741-3335

Abstract

Abstract: In a recent article by Li et al (2019 Sci. 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 (∝1/ λ 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 ∼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 ∼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.