Laser-driven collisionless shock acceleration of protons from gas jets tailored by one or two nanosecond beams

2021 ◽  
Vol 28 (11) ◽  
pp. 113102
Author(s):  
J. Bonvalet ◽  
P. Loiseau ◽  
J.-R. Marquès ◽  
E. Atukpor ◽  
E. d'Humières ◽  
...  
2016 ◽  
Vol 23 (5) ◽  
pp. 053103 ◽  
Author(s):  
B. Svedung Wettervik ◽  
T. C. DuBois ◽  
T. Fülöp

2019 ◽  
Vol 26 (12) ◽  
pp. 123102
Author(s):  
R. Xie ◽  
L. H. Cao ◽  
J. X. Gong ◽  
H. Cheng ◽  
Z. J. Liu ◽  
...  

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Prashant Kumar Singh ◽  
Vishwa Bandhu Pathak ◽  
Jung Hun Shin ◽  
Il Woo Choi ◽  
Kazuhisa Nakajima ◽  
...  

Abstract With the recent advances in ultrahigh intensity lasers, exotic astrophysical phenomena can be investigated in laboratory environments. Collisionless shock in a plasma, prevalent in astrophysical events, is produced when a strong electric or electromagnetic force induces a shock structure in a time scale shorter than the collision time of charged particles. A near-critical-density (NCD) plasma, generated with an intense femtosecond laser, can be utilized to excite a collisionless shock due to its efficient and rapid energy absorption. We present electrostatic shock acceleration (ESA) in experiments performed with a high-density helium gas jet, containing a small fraction of hydrogen, irradiated with a 30 fs, petawatt laser. The onset of ESA exhibited a strong dependence on plasma density, consistent with the result of particle-in-cell simulations on relativistic plasma dynamics. The mass-dependent ESA in the NCD plasma, confirmed by the preferential reflection of only protons with two times the shock velocity, opens a new possibility of selective acceleration of ions by electrostatic shock.


2016 ◽  
Author(s):  
N. Cook ◽  
O. Tresca ◽  
N. P. Dover ◽  
C. Maharjan ◽  
M. N. Polyanskiy ◽  
...  

2021 ◽  
Vol 2021 ◽  
pp. 1-9
Author(s):  
Yue Chao ◽  
Xinxin Yan ◽  
Rui Xie ◽  
Lihua Cao ◽  
Chunyang Zheng ◽  
...  

Effects of solid nanolayers embedded in a near-critical density plasma on the laser-driven collisionless shock acceleration are investigated by using two-dimensional particle-in-cell simulations. Due to the interaction of nanolayers and the incident laser, an additional number of hot electrons are generated and an inhomogeneous magnetic field is induced. As a result, the collisionless shock is reinforced within the nanolayer gaps compared to the target without the structured nanolayers. When the laser intensity is 9.8 × 10 19  W / cm 2 , the amplitude of the electrostatic field is increased by 30% and the shock velocity is increased from 0.079c to 0.091c, leading to an enhancement of the peak energy and the cutoff energy of accelerated protons, from 6.9 MeV to 9.1 MeV and 12.2 MeV to 20.0 MeV, respectively. Furthermore, the effects of the width of the nanolayer gaps are studied, by adjusting the gap width of nanolayers, and optimal nanolayer setups for collisionless shock acceleration can be acquired.


2020 ◽  
Vol 27 (8) ◽  
pp. 083102 ◽  
Author(s):  
S. Tochitsky ◽  
A. Pak ◽  
F. Fiuza ◽  
D. Haberberger ◽  
N. Lemos ◽  
...  

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