MeV-order proton and carbon ion acceleration by irradiation of 60 fs TW laser pulses on thin copper tape

2003 ◽  
Vol 83 (8) ◽  
pp. 1524-1526 ◽  
Author(s):  
Takashi Fujii ◽  
Yuji Oishi ◽  
Takuya Nayuki ◽  
Yasushi Takizawa ◽  
Koshichi Nemoto ◽  
...  
2019 ◽  
Vol 37 (4) ◽  
pp. 346-353
Author(s):  
D. Sangwan ◽  
O. Culfa ◽  
C.P. Ridgers ◽  
S. Aogaki ◽  
D. Stutman ◽  
...  

AbstractWe present results of 2D particle-in-cell (PIC) simulations of carbon ion acceleration by 10 petawatt (PW) laser pulses, studying both circular polarized (CP) and linear polarized (LP) pulses. We carry out a thickness scanning of a solid carbon target to investigate the ideal thickness for carbon ion acceleration mechanisms using a 10 PW laser with an irradiance of 5 × 1022 W cm−2. The energy spectra of carbon ions and electrons and their temperature are studied. Additionally, for the carbon ions, their angular divergence is studied. It is shown that the ideal thickness for the carbon acceleration is 120 nm and the cutoff energy for carbon ions is 5 and 3 GeV for CP and LP pulses, respectively. The corresponding carbon ions temperature is ~1 and ~0.75 GeV. On the other hand, the energy cutoff for the electrons is ~500 MeV with LP and ~400 MeV with CP laser pulses. We report that the breakout afterburner mechanism is most likely causing the acceleration of carbon ions to such high energies for the optimal target thickness.


2015 ◽  
Vol 5 (1) ◽  
Author(s):  
Malay Dalui ◽  
W.-M. Wang ◽  
T. Madhu Trivikram ◽  
Subhrangsu Sarkar ◽  
Sheroy Tata ◽  
...  

Abstract High-intensity ultrashort laser pulses focused on metal targets readily generate hot dense plasmas which accelerate ions efficiently and can pave way to compact table-top accelerators. Laser-driven ion acceleration studies predominantly focus on protons, which experience the maximum acceleration owing to their highest charge-to-mass ratio. The possibility of tailoring such schemes for the preferential acceleration of a particular ion species is very much desired but has hardly been explored. Here, we present an experimental demonstration of how the nanostructuring of a copper target can be optimized for enhanced carbon ion acceleration over protons or Cu-ions. Specifically, a thin (≈0.25 μm) layer of 25–30 nm diameter Cu nanoparticles, sputter-deposited on a polished Cu-substrate, enhances the carbon ion energy by about 10-fold at a laser intensity of 1.2×1018  W/cm2. However, particles smaller than 20 nm have an adverse effect on the ion acceleration. Particle-in-cell simulations provide definite pointers regarding the size of nanoparticles necessary for maximizing the ion acceleration. The inherent contrast of the laser pulse is found to play an important role in the species selective ion acceleration.


2010 ◽  
Vol 12 (4) ◽  
pp. 045020 ◽  
Author(s):  
D C Carroll ◽  
O Tresca ◽  
R Prasad ◽  
L Romagnani ◽  
P S Foster ◽  
...  

2021 ◽  
Vol 28 (2) ◽  
pp. 023102
Author(s):  
X. Z. Wu ◽  
Z. Gong ◽  
Y. R. Shou ◽  
Y. H. Tang ◽  
J. Q. Yu ◽  
...  

2009 ◽  
Vol 16 (8) ◽  
pp. 083103 ◽  
Author(s):  
T. Schlegel ◽  
N. Naumova ◽  
V. T. Tikhonchuk ◽  
C. Labaune ◽  
I. V. Sokolov ◽  
...  

2018 ◽  
Vol 25 (8) ◽  
pp. 083113 ◽  
Author(s):  
M. Tayyab ◽  
S. Bagchi ◽  
J. A. Chakera ◽  
R. A. Khan ◽  
P. A. Naik

2019 ◽  
Vol 61 (11) ◽  
pp. 115005
Author(s):  
H He ◽  
B Qiao ◽  
X F Shen ◽  
W P Yao ◽  
Y L Yao ◽  
...  

Author(s):  
J. Hornung ◽  
Y. Zobus ◽  
P. Boller ◽  
C. Brabetz ◽  
U. Eisenbarth ◽  
...  

We present a study of laser-driven ion acceleration with micrometre and sub-micrometre thick targets, which focuses on the enhancement of the maximum proton energy and the total number of accelerated particles at the PHELIX facility. Using laser pulses with a nanosecond temporal contrast of up to $10^{-12}$ and an intensity of the order of $10^{20}~\text{W}/\text{cm}^{2}$ , proton energies up to 93 MeV are achieved. Additionally, the conversion efficiency at $45^{\circ }$ incidence angle was increased when changing the laser polarization to p, enabling similar proton energies and particle numbers as in the case of normal incidence and s-polarization, but reducing the debris on the last focusing optic.


2011 ◽  
Vol 99 (12) ◽  
pp. 121504 ◽  
Author(s):  
R. Prasad ◽  
A. A. Andreev ◽  
S. Ter-Avetisyan ◽  
D. Doria ◽  
K. E. Quinn ◽  
...  

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