A new high intensity and short-pulse molecular beam valve

2013 ◽  
Vol 84 (2) ◽  
pp. 023102 ◽  
Author(s):  
B. Yan ◽  
P. F. H. Claus ◽  
B. G. M. van Oorschot ◽  
L. Gerritsen ◽  
A. T. J. B. Eppink ◽  
...  
2014 ◽  
Vol 85 (11) ◽  
pp. 116107 ◽  
Author(s):  
Chamara Abeysekera ◽  
Baptiste Joalland ◽  
Yuanyuan Shi ◽  
Alexander Kamasah ◽  
James M. Oldham ◽  
...  

1963 ◽  
Vol 34 (1) ◽  
pp. 96-100 ◽  
Author(s):  
J. Deckers ◽  
J. B. Fenn

2011 ◽  
Vol 18 (10) ◽  
pp. 103103 ◽  
Author(s):  
Alexander Andreev ◽  
Naveen Kumar ◽  
Konstantin Platonov ◽  
Alexander Pukhov

2018 ◽  
Vol 89 (11) ◽  
pp. 115106 ◽  
Author(s):  
Genbai Chu ◽  
Tao Xi ◽  
Minghai Yu ◽  
Wei Fan ◽  
Yongqiang Zhao ◽  
...  

2002 ◽  
Vol 20 (2) ◽  
pp. 321-336 ◽  
Author(s):  
DIMITRI BATANI

The paper reviews and analyses the experiments devoted to the propagation in dense matter of fast electrons produced in the interaction of short-pulse ultra-high-intensity laser pulses with solid density targets.


Crystals ◽  
2020 ◽  
Vol 10 (9) ◽  
pp. 783
Author(s):  
Hiromitsu Kiriyama ◽  
Alexander S. Pirozhkov ◽  
Mamiko Nishiuchi ◽  
Yuji Fukuda ◽  
Akito Sagisaka ◽  
...  

Ultra-high intensity femtosecond lasers have now become excellent scientific tools for the study of extreme material states in small-scale laboratory settings. The invention of chirped-pulse amplification (CPA) combined with titanium-doped sapphire (Ti:sapphire) crystals have enabled realization of such lasers. The pursuit of ultra-high intensity science and applications is driving worldwide development of new capabilities. A petawatt (PW = 1015 W), femtosecond (fs = 10−15 s), repetitive (0.1 Hz), high beam quality J-KAREN-P (Japan Kansai Advanced Relativistic ENgineering Petawatt) Ti:sapphire CPA laser has been recently constructed and used for accelerating charged particles (ions and electrons) and generating coherent and incoherent ultra-short-pulse, high-energy photon (X-ray) radiation. Ultra-high intensities of 1022 W/cm2 with high temporal contrast of 10−12 and a minimal number of pre-pulses on target has been demonstrated with the J-KAREN-P laser. Here, worldwide ultra-high intensity laser development is summarized, the output performance and spatiotemporal quality improvement of the J-KAREN-P laser are described, and some experimental results are briefly introduced.


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