2022
DOI: 10.1063/5.0090514
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Commissioning and first results from the new 2 × 100 TW laser at the WIS

Abstract: At the Weizmann Institute of Science, a new high-power-laser laboratory has been established that is dedicated to the fundamental aspects of laser–matter interaction in the relativistic regime and aimed at developing compact laser-plasma accelerators for delivering high-brightness beams of electrons, ions, and x rays. The HIGGINS laser system delivers two independent 100 TW beams and an additional probe beam, and this paper describes its commissioning and presents the very first results for particle and radiat… Show more

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Cited by 13 publications
(7 citation statements)
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“…Concerning the literature, we also would like to recall that with a similar laser system, with a longer off-axis parabola, and similar conditions for plasma density and injection scheme, other authors have demonstrated the same electron energies but higher critical energy (in the few keVs) and number of photons (∼10 8 ) [26]. In another work, with a similar experimental setup, larger electron energies up to 500 MeV have been demonstrated and larger critical energies of the betatron spectrum up to 10 keV [35], but smaller bunch charges. The reason for these differences may be attributed to different conditions for laser guiding and/or different injection schemes realized, e.g., with a mixture of gases, affecting the electron beam emittance, the bunch charge and the energy spread.…”
Section: Discussionmentioning
confidence: 59%
“…Concerning the literature, we also would like to recall that with a similar laser system, with a longer off-axis parabola, and similar conditions for plasma density and injection scheme, other authors have demonstrated the same electron energies but higher critical energy (in the few keVs) and number of photons (∼10 8 ) [26]. In another work, with a similar experimental setup, larger electron energies up to 500 MeV have been demonstrated and larger critical energies of the betatron spectrum up to 10 keV [35], but smaller bunch charges. The reason for these differences may be attributed to different conditions for laser guiding and/or different injection schemes realized, e.g., with a mixture of gases, affecting the electron beam emittance, the bunch charge and the energy spread.…”
Section: Discussionmentioning
confidence: 59%
“…The experiment was conducted using the HIGGINS dual 100-TW laser system at the Weizmann Institute of Science ( 37 ). In the experimental setup, one laser beam with 1.2-J and 30-fs duration was focused onto a 3-mm-long helium gas jet doped with 1% nitrogen, resulting in the stable production of an ultra-relativistic electron bunch as a probe.…”
Section: Resultsmentioning
confidence: 99%
“…The experiment was carried out at the HIGGINS dual 100-TW laser platform at the Weizmann Institute of Science ( 37 ), where a 1-Hz, 7-J laser beam was split into two equal parts after the final amplifier: laser A for the acceleration of the probe electron bunch, and laser B for driving the wakefield. Both lasers were independently compressed to 30-fs durations and focused to 28.5- and 37.8-μm spots (FWHM), respectively.…”
Section: Methodsmentioning
confidence: 99%
“…To validate the proposed method, we performed the experiment at the HIGGINS dual 100 TW laser platform of the Weizmann Institute of Science 33 . The LPA-generated electron bunch that was investigated was obtained by focusing a 0.8 J, 30 fs laser beam onto a 5-mm diameter supersonic gas jet using a mixture of helium and nitrogen with a plasma density of 4 × 10 18 cm −3 in the plateau.…”
Section: Resultsmentioning
confidence: 99%
“…The experiment was carried out using the HIGGINS dual 100 TW laser system at the Weizmann Institute of Science 33 . The HIGGINS system is comprised of two separate laser pulses (A and B) split from a 7 J laser.…”
Section: Methodsmentioning
confidence: 99%