scholarly journals Solid-target seeded soft X-ray laser for short pulses and optical vortex amplification

Author(s):  
Olivier Guilbaud ◽  
Alok-Kumar Pandey ◽  
Elsa Baynard ◽  
Irene papagiannouli ◽  
Fabrice Sanson ◽  
...  
2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Evgeny D. Filippov ◽  
Sergey S. Makarov ◽  
Konstantin F. Burdonov ◽  
Weipeng Yao ◽  
Guilhem Revet ◽  
...  

AbstractWe analyze, using experiments and 3D MHD numerical simulations, the dynamic and radiative properties of a plasma ablated by a laser (1 ns, 10$$^{12}$$ 12 –10$$^{13}$$ 13 W/cm$$^2$$ 2 ) from a solid target as it expands into a homogeneous, strong magnetic field (up to 30 T) that is transverse to its main expansion axis. We find that as early as 2 ns after the start of the expansion, the plasma becomes constrained by the magnetic field. As the magnetic field strength is increased, more plasma is confined close to the target and is heated by magnetic compression. We also observe that after $$\sim 8$$ ∼ 8  ns, the plasma is being overall shaped in a slab, with the plasma being compressed perpendicularly to the magnetic field, and being extended along the magnetic field direction. This dense slab rapidly expands into vacuum; however, it contains only $$\sim 2\%$$ ∼ 2 % of the total plasma. As a result of the higher density and increased heating of the plasma confined against the laser-irradiated solid target, there is a net enhancement of the total X-ray emissivity induced by the magnetization.


Author(s):  
Ibrahim R. Agool ◽  
Ahmed N. Abd ◽  
Mohammed O. Dawood

Nanoparticles NPSof cadmium oxide CdO were generated by laser ablation of a solid target (cadmium) in polyvinylpyrrolidone (PVP) solution. CdO colloidal nanoparticles have been synthesized by laser ablation Nd:YAG (1064 nm, 100 pulses, pulse energy= 400 mJ) when the solid target CdO was immersed in PVP. Structure, topography and optical properties of the CdO nanoparticles NPShave been studied using X-ray diffraction (XRD), atomic force microscope (AFM) and the UV-Vis absorption respectively.


2020 ◽  
Vol 28 (20) ◽  
pp. 28924
Author(s):  
Alok Kumar Pandey ◽  
Irene Papagiannouli ◽  
Fabrice Sanson ◽  
Elsa Baynard ◽  
Julien Demailly ◽  
...  

2014 ◽  
Vol 26 (11) ◽  
pp. 112001
Author(s):  
胡青元 Hu Qingyuan ◽  
杨军 Yang Jun ◽  
甯家敏 Ning Jiamin ◽  
甫跃成 Fu Yuecheng ◽  
杨建伦 Yang Jianlun ◽  
...  
Keyword(s):  

Author(s):  
D. Ursescu ◽  
G. Cojocaru ◽  
R. Ungureanu ◽  
R Banici ◽  
L. Ionel ◽  
...  
Keyword(s):  

2005 ◽  
Author(s):  
Hiroto Kuroda ◽  
Rashid Ganeev ◽  
Masayuki Suzuki ◽  
Motoyoshi Baba ◽  
Jun Zhang ◽  
...  

1995 ◽  
Vol 377 ◽  
Author(s):  
H. K. Lee ◽  
J. S. Drewery ◽  
W. S. Hone ◽  
T. Jing ◽  
S. N. Kaplan ◽  
...  

ABSTRACTThe photoconductive gain mechanism in a-Si:H was investigated in connection with applications to radiation detection. Various device types such as p-i-n, n-i-n and n-i-p-i-n structures were fabricated and tested. Photoconductive gain was measured in two time scales: one for short pulses of visible light (< 1 μsec) which simulates the transit of an energetic charged particle, and the other for rather long pulses of light (1 msec) which simulates x-ray exposure in medical imaging. We used two definitions of photoconductive gain: current gain and charge gain which is an integration of the current gain. We found typical charge gains of 3 ∼ 9 for short pulses and a few hundred for long pulses at a dark current level of 10 mA/cm2. Various gain results are discussed in terms of the device structure, applied bias and dark current.


Author(s):  
W.S. Graves ◽  
M. Farkhondeb ◽  
F.X. Kaortner ◽  
R. Milner ◽  
C. Tschalaer ◽  
...  
Keyword(s):  
X Ray ◽  

2013 ◽  
Vol 38 (20) ◽  
pp. 4011 ◽  
Author(s):  
Lu Li ◽  
Yong Wang ◽  
Shoujun Wang ◽  
Eduardo Oliva ◽  
Liang Yin ◽  
...  
Keyword(s):  
X Ray ◽  

2014 ◽  
Vol 70 (a1) ◽  
pp. C296-C296
Author(s):  
John Spence

"The NSF BioXFEL Science and Technology Center (STC) is a new consortium of six research campuses devoted to the application of x-ray free-electron lasers (XFELs) to structural biology. Over the last four years a variety of approaches have been made to the observation of protein structure and dynamics for various classes of proteins. The Linac Coherent Light source at SLAC, the first hard-Xray EXFEL, provides intense coherent hard X-ray pulses at 120 Hz which vaporize protein when focussed to a sub-micron beam. Atomic-resolution Bragg diffraction patterns are nevertheless obtained using 50 fs pulses prior to the onset of significant damage, in this ""diffract-then-destroy"" mode, which outruns radiation damage. This use of short pulses instead of freezing samples to reduce radiation damage therefore opens the way to the study of protein dynamics at room temperature in a native environment. I'll review the work of several groups using a range of approaches to different types of sample, including the following: 1. Differences between the frozen sychrotron structure of GPCR proteins and the RT XFEL structure [1]. 2. Pump-probe dynamic structures in Photosynthesis [2]. 3. XFEL study of 2D protein crystals [3]. 4. Prospects for improved resolution in XFEL imaging from single particles such as viruses, where patterns can be obtained from a single virus. 5. New ideas - the Lipid Cubic Phase injector (which allows protein nanocrystals to be studied also at sychrotrons) [4], prospects for fast Laue diffraction using coherent attosecond X-ray lasers, ab-initio phasing [5], the use of angular correlation functions for analysis of fast solution scattering, and two-color opportunites for serial femtosecond crystallography (SFX). See [6] for a recent review of the field. 1. W.Liu et al Science 342, 1521 (2013) 2. A.Aquila et al Optics Express 20, 2706 (2012) 3. M.Frank et al IUCrJ (2014) In press. 4. U.Weierstall et al Nature Comms. (2014) In press. 5. J. Spence et al Optics Express 19, 2866 (2011). 6. J. Spence et al Rep. Prog. Phys. 75, 102601 (2012)."


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