Temperature Measurements of Plasmas Produced by Laser Pulses in Gas Jets

1971 ◽  
Vol 19 (8) ◽  
pp. 300-302 ◽  
Author(s):  
H. J. Neusser ◽  
H. Puell ◽  
W. Kaiser
2012 ◽  
Author(s):  
Yuji Oishi ◽  
Takuya Nayuki ◽  
Alexei Zhidkov ◽  
Takashi Fujii ◽  
Koshichi Nemoto

2011 ◽  
Vol 50 (4R) ◽  
pp. 042702 ◽  
Author(s):  
Yuji Oishi ◽  
Takuya Nayuki ◽  
Alexei Zhidkov ◽  
Takashi Fujii ◽  
Koshichi Nemoto

2017 ◽  
Author(s):  
K. K. Swanson ◽  
H.-E. Tsai ◽  
S. K. Barber ◽  
R. Lehe ◽  
H.-S. Mao ◽  
...  

2011 ◽  
Vol 50 (4) ◽  
pp. 042702 ◽  
Author(s):  
Yuji Oishi ◽  
Takuya Nayuki ◽  
Alexei Zhidkov ◽  
Takashi Fujii ◽  
Koshichi Nemoto

2020 ◽  
Vol 8 ◽  
Author(s):  
Maria Alkhimova ◽  
Sergey Ryazantsev ◽  
Igor Skobelev ◽  
Alexey Boldarev ◽  
Jie Feng ◽  
...  

In this work, we optimized a clean, versatile, compact source of soft X-ray radiation $(E_{\text{x}\text{-}\text{ray}}\sim 3~\text{keV})$ with an yield per shot up to $7\times 10^{11}~\text{photons}/\text{shot}$ in a plasma generated by the interaction of high-contrast femtosecond laser pulses of relativistic intensity $(I_{\text{las}}\sim 10^{18}{-}10^{19}~\text{W}/\text{cm}^{2})$ with supersonic argon gas jets. Using high-resolution X-ray spectroscopy approaches, the dependence of main characteristics (temperature, density and ionization composition) and the emission efficiency of the X-ray source on laser pulse parameters and properties of the gas medium was studied. The optimal conditions, when the X-ray photon yield reached a maximum value, have been found when the argon plasma has an electron temperature of $T_{\text{e}}\sim 185~\text{eV}$ , an electron density of $N_{\text{e}}\sim 7\times 10^{20}~\text{cm}^{-3}$ and an average charge of $Z\sim 14$ . In such a plasma, a coefficient of conversion to soft X-ray radiation with energies $E_{\text{x}\text{-}\text{ray}}\sim 3.1\;(\pm 0.2)~\text{keV}$ reaches $8.57\times 10^{-5}$ , and no processes leading to the acceleration of electrons to MeV energies occur. It was found that the efficiency of the X-ray emission of this plasma source is mainly determined by the focusing geometry. We confirmed experimentally that the angular distribution of the X-ray radiation is isotropic, and its intensity linearly depends on the energy of the laser pulse, which was varied in the range of 50–280 mJ. We also found that the yield of X-ray photons can be notably increased by, for example, choosing the optimal laser pulse duration and the inlet pressure of the gas jet.


2020 ◽  
Vol 46 (3) ◽  
pp. 275-278
Author(s):  
M. A. Alkhimova ◽  
S. N. Ryazantsev ◽  
I. Yu. Skobelev ◽  
M. D. Mishchenko ◽  
A. S. Boldarev ◽  
...  

2013 ◽  
Vol 479-480 ◽  
pp. 91-95
Author(s):  
Jin Chen Hsu ◽  
Cheng Yun Liao ◽  
Chao Ching Ho ◽  
Yuan Jen Chang ◽  
Chia Lung Kuo

In this paper, intermittent gas jet assisted laser drilling on stainless steel (SUS304) with a fiber laser of wavelength 1090 nm is studied. Compared with the conventionally used continuous gas jets in assisting laser drilling, the intermittent gas jet assisting can effectively increase the material removal rate. The intermittent gas jet can be modulated with the frequency to effectively reduce the over-cooling effect by the assist gas. Experimental result shows that the drilling depth and machining time can be improved. The effects of the intermittent gas jet pressures and the synchronicity of gas and laser pulses on the laser drilling are investigated and discussed. It is observed that the intermittent gas jet method obviously reduces heat loss and increases the machining efficiency during the laser drilling. Compared with result of using the continuous gas jet, laser drilling with the intermittent gas jet at 40 Hz increases the drilling depth with an improvement of 10%. It is worth noting that the intermittent gas jet method can also reduce the quantity and cost of gas while the gases such as helium and argon gases are applied.


2002 ◽  
Vol 12 (3) ◽  
pp. 201-206 ◽  
Author(s):  
Janina Marciak-Kozłowska ◽  
Mirosław Kozłowski
Keyword(s):  

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