Abstract:We report results of an experimental study of laser-wakefield acceleration of electrons, using a staged device based on a double-jet gas target that enables independent injection and acceleration stages. This novel scheme is shown to produce stable, quasi-monoenergetic, and tunable electron beams. We show that optimal accelerator performance is achieved by systematic variation of five critical parameters. For the injection stage, we show that the amount of trapped charge is controlled by the gas density, compo… Show more
“…Advanced acceleration techniques are being pursued via different approaches, aiming at compact, more affordable systems to drive secondary radiation sources [1][2][3][4][5][6][7][8][9][10] or even future particle colliders [11][12][13]. In this context, laser wakefield acceleration (LWFA) of electrons offers a very promising path, with experiments showing further increase of maximum energy, now approaching 8 GeV [14], including staging exploration [15][16][17][18][19] and high repetition rate operation at the lower energy end [20]. In view of the construction of the first user facility based on plasma acceleration, effort is now directed toward the demonstration of stable operation of a GeV scale electron beam at high specification, as those needed for an x-ray free electron laser (FEL) in the EuPRAXIA project [21].…”
Laser wakefield acceleration of GeV electrons is becoming a mature technique, so that a reliable accelerator delivering stable beams to users communities can now be considered. In such a context, two plasma stages, one injector and one booster stage, offer a flexible solution for optimization. For the injector we consider here the resonant multipulse ionization injection (ReMPI) that can be optimized to generate electron bunches with high enough quality to be efficiently transported to the second stage. In order to better control the beam-loading effect and optimize the beam manipulation after the plasma downramp, a quasiround beam is preferable. In this respect, we present analytical and particle-in-cell results concerning the tunnel-ionization process in presence of two, orthogonally polarized, laser pulses with different wavelengths. We also show, by means of hybrid fluid/PIC numerical simulations, that a stable working point with the ReMPI injector exists at 32 pC, 4 kA peak current, with mean energy of 150 MeV, energy spread of 1.65% rms, normalized emittance Ļµ n Ā¼ 0.23 Ī¼m and divergence of 0.6 mrad. The scheme relies on a 150 TW Ti:Sa laser modified to achieve a four-pulses driver train and a third harmonics ionization pulse.
“…Advanced acceleration techniques are being pursued via different approaches, aiming at compact, more affordable systems to drive secondary radiation sources [1][2][3][4][5][6][7][8][9][10] or even future particle colliders [11][12][13]. In this context, laser wakefield acceleration (LWFA) of electrons offers a very promising path, with experiments showing further increase of maximum energy, now approaching 8 GeV [14], including staging exploration [15][16][17][18][19] and high repetition rate operation at the lower energy end [20]. In view of the construction of the first user facility based on plasma acceleration, effort is now directed toward the demonstration of stable operation of a GeV scale electron beam at high specification, as those needed for an x-ray free electron laser (FEL) in the EuPRAXIA project [21].…”
Laser wakefield acceleration of GeV electrons is becoming a mature technique, so that a reliable accelerator delivering stable beams to users communities can now be considered. In such a context, two plasma stages, one injector and one booster stage, offer a flexible solution for optimization. For the injector we consider here the resonant multipulse ionization injection (ReMPI) that can be optimized to generate electron bunches with high enough quality to be efficiently transported to the second stage. In order to better control the beam-loading effect and optimize the beam manipulation after the plasma downramp, a quasiround beam is preferable. In this respect, we present analytical and particle-in-cell results concerning the tunnel-ionization process in presence of two, orthogonally polarized, laser pulses with different wavelengths. We also show, by means of hybrid fluid/PIC numerical simulations, that a stable working point with the ReMPI injector exists at 32 pC, 4 kA peak current, with mean energy of 150 MeV, energy spread of 1.65% rms, normalized emittance Ļµ n Ā¼ 0.23 Ī¼m and divergence of 0.6 mrad. The scheme relies on a 150 TW Ti:Sa laser modified to achieve a four-pulses driver train and a third harmonics ionization pulse.
“…This technique, providing potentially jitter-free sources of radiation and electrons, has already demonstrated the electron acceleration over 4 GeV [13] in a single stage with laser pulse energy less than 100 J. However, similar to vacuum acceleration schemes, the staging schemes in plasma (an injector, a buster, and so on) seem to be more practical providing better stability and reproducibility of the acceleration process [17,18].…”
Staging laser wake-field acceleration is considered to be a necessary technique for developing full-optical jitter-free high energy electron accelerators. Splitting of the acceleration length into several technical parts and with independent laser drivers allows not only the generation of stable, reproducible acceleration fields but also overcoming the dephasing length while maintaining an overall high acceleration gradient and a compact footprint. Temporal and spatial coupling of pre-accelerated electron bunches for their injection in the acceleration phase of a successive laser pulse wake field is the key part of the staging laser-driven acceleration. Here, characterization of the coupling is performed with a dense, stable, narrow energy band of <3% and energy-selectable electron beams with a charge of ~1.6 pC and energy of ~10āMeV generated from a laser plasma cathode. Cumulative focusing of electron bunches in a low-density preplasma, exhibiting the BudkerāBennett effect, is shown to result in the efficient injection of electrons, even with a long distance between the injector and the booster in the laser pulse wake. The measured characteristics of electron beams modified by the booster wake field agree well with those obtained by multidimensional particle-in-cell simulations.
“…High-quality Laser Wake Field Accelerated (LWFA) electron bunches are nowdays requested for several applications including Free Electron Lasers [1][2][3], X/Ī³ radiation sources [4][5][6][7][8] and staged acceleration [9][10][11][12][13]. While performances of self-injected bunches generated in the socalled bubble-regime [14,15] continue to improve, other promising injection schemes, including injection via density downramp [16][17][18][19][20], colliding pulses injection [21][22][23] and ionization injection [24][25][26][27][28][29][30][31][32], are under active theoretical and experimental investigation.…”
The production of high-quality electron bunches in Laser Wake Field Acceleration relies on the possibility to inject ultra-low emittance bunches in the plasma wave. In this paper we present a new bunch injection scheme in which electrons extracted by ionization are trapped by a large-amplitude plasma wave driven by a train of resonant ultrashort pulses. In the REsonant Multi-Pulse Ionization (REMPI) injection scheme, the main portion of a single ultrashort (e.g Ti:Sa) laser system pulse is temporally shaped as a sequence of resonant sub-pulses, while a minor portion acts as an ionizing pulse. Simulations show that high-quality electron bunches with normalized emittance as low as 0.08 mmĆmrad and 0.65% energy spread can be obtained with a single present-day 100TW-class Ti:Sa laser system.
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