Observations of the intense soft x-ray emissions from ultrathin Au films irradiated with high contrast laser pulses

2010 ◽  
Author(s):  
Masahiko Ishino ◽  
Masataka Kado ◽  
Masaharu Nishikino ◽  
Kunio Shinohara ◽  
Satoshi Tamotsu ◽  
...  
Keyword(s):  
2004 ◽  
Vol 22 (3) ◽  
pp. 301-306 ◽  
Author(s):  
S.A. GAVRILOV ◽  
D.M. GOLISHNIKOV ◽  
V.M. GORDIENKO ◽  
A.B. SAVEL'EV ◽  
R.V. VOLKOV

Recent results on constructing of an efficient hard X-ray source using solid targets irradiated by high-contrast 200-fs laser pulses with an intensity above 1016W/cm2are presented. We used different solid targets with a laser- and electrochemically modified surface layer: craters, pyramidal cavities, porous silicon, gratings. Experimental data obtained confirms that using solid targets with a corrugated surface one can achieve a prominent increase both in the efficiency of hard X-ray generation (in the quanta range 2–30 keV) and in the hot electron temperature of plasma.


2022 ◽  
Vol 29 (1) ◽  
pp. 013301
Author(s):  
E. Eftekhari-Zadeh ◽  
M. S. Blümcke ◽  
Z. Samsonova ◽  
R. Loetzsch ◽  
I. Uschmann ◽  
...  

2013 ◽  
Vol 9 (3) ◽  
pp. 560-567 ◽  
Author(s):  
S.A. Pikuz ◽  
A.Ya. Faenov ◽  
J. Colgan ◽  
R.J. Dance ◽  
J. Abdallah ◽  
...  

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 ◽  
...  

Author(s):  
М.А. Алхимова ◽  
С.Н. Рязанцев ◽  
И.Ю. Скобелев ◽  
М.Д. Мищенко ◽  
А.C. Болдарев ◽  
...  

We investigated the opportunity to create a soft X-ray source in laser-produced plasma without concomitant fast electrons generation. The x-ray source has been created under the interaction of high-contrast relativistic femtosecond laser pulses with super-sonic Argon jets. Optimal conditions when conversion coefficient to soft x-ray at the range 2.9 – 3.3 keV reached 8.57 ·10^(-5) have been found.


1995 ◽  
Vol 2 (5) ◽  
pp. 1702-1711 ◽  
Author(s):  
Z. Jiang ◽  
J. C. Kieffer ◽  
J. P. Matte ◽  
M. Chaker ◽  
O. Peyrusse ◽  
...  

Author(s):  
Uwe Lücken ◽  
Michael Felsmann ◽  
Wim M. Busing ◽  
Frank de Jong

A new microscope for the study of life science specimen has been developed. Special attention has been given to the problems of unstained samples, cryo-specimens and x-ray analysis at low concentrations.A new objective lens with a Cs of 6.2 mm and a focal length of 5.9 mm for high-contrast imaging has been developed. The contrast of a TWIN lens (f = 2.8 mm, Cs = 2 mm) and the BioTWTN are compared at the level of mean and SD of slow scan CCD images. Figure 1a shows 500 +/- 150 and Fig. 1b only 500 +/- 40 counts/pixel. The contrast-forming mechanism for amplitude contrast is dependent on the wavelength, the objective aperture and the focal length. For similar image conditions (same voltage, same objective aperture) the BioTWIN shows more than double the contrast of the TWIN lens. For phasecontrast specimens (like thin frozen-hydrated films) the contrast at Scherzer focus is approximately proportional to the √ Cs.


2001 ◽  
Vol 11 (PR2) ◽  
pp. Pr2-39-Pr2-42 ◽  
Author(s):  
M. Kado ◽  
T. Kawachi ◽  
N. Hasegawa ◽  
M. Tanaka ◽  
K. Sukegawa ◽  
...  

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