Laser plasma studies using a high-power 249-nm KrF laser

1985 ◽  
Author(s):  
F. O’NEILL ◽  
M. J. SHAW ◽  
M. H. KEY ◽  
I. N. ROSS ◽  
F. KANNARI ◽  
...  
Keyword(s):  
1983 ◽  
Author(s):  
C. B. Edwards ◽  
F. O’Neill ◽  
M. J. Shaw ◽  
D. Baker ◽  
D. Craddock ◽  
...  
Keyword(s):  

2002 ◽  
Author(s):  
Zhenhuan Ye ◽  
Qihong Lou ◽  
Jingxing Dong ◽  
Lei Lin
Keyword(s):  

1986 ◽  
Vol 75 ◽  
Author(s):  
Harold M. Anderson ◽  
Philip J. Hargis

AbstractA model for dendrite growths in polycrystalline Si films formed during laser/plasma deposition with a silane discharge and a pulsed KrF laser has been developed. The model assumes a thin (less than 10 nm) amorphous silicon (a-Si) film is deposited on a substrate prior to phase transformation due to laser heating. The observed dendritic structure of the overall polycrystalline Si films is attributed to Si crystals shooting from an excessively supercooled Si liquid bath. Supercooled liquid forms since the melting point for a-Si can be reached at relatively low KrF laser fluences. Latent heat evolved at the solid-liquid interface induces an interface temperature higher than that of the melt and the requisite negative temperature gradient for absolute bath supercooling. Since the formation of an undercooled liquid by fast melting a-Si is also an important first step in explosive crystal regrowth studies, these results may have important implications for crystal growth and transient annealing. A conical approximation model is used in this study to characterize the stability of the dendrite tip in terms of local temperature gradients, i.e., the degree of undercooling at the tip of the parabolic dendrite. The degree of undercooling and hence the tip radius appears to be significantly affected by small changes in the laser fluence. Stability criteria lead to a relationship between regrowth velocity, V, and the tip radius, R, of the form VR2= constant. The size and stability of the dendrite tip is determined from a balance between the destabilizing force due to thermal diffusion and the stabilizing capillary force. Based on the observed tip radii formed at laser fluences from 0.13 to 0.25 J/cm2, the model predicts regrowth velocities in a range between 2.0 and 20 m/s – values consistent with transient annealing studies of a-Si


2021 ◽  
Vol 9 ◽  
Author(s):  
Yumi Kaneyasu ◽  
Keiji Nagai ◽  
Marilou Cadatal-Raduban ◽  
Daniil Golovin ◽  
Satoshi Shokita ◽  
...  

Abstract Resorcinol/formaldehyde (RF) foam resin is an attractive material as a low-density target in high-power laser–plasma experiments because of its fine network structure, transparency in the visible region, and low-Z element (hydrogen, carbon, and oxygen) composition. In this study, we developed disk-shaped RF foam and deuterated RF foam targets with 40–200 μm thickness and approximately 100 mg/cm3 density having a network structure from 100 nm to a few micrometers cell size. By deuteration, the polymerization rate was drastically slowed down owing to kinetic isotope effects. These targets were used in high-power laser experiments where a megaelectronvolt proton beam was successfully generated.


1988 ◽  
Author(s):  
I C. E. Turcu ◽  
F O'Neill ◽  
U Zammit ◽  
Y Al-Hadithi ◽  
R W. Eason ◽  
...  
Keyword(s):  
X Ray ◽  

2015 ◽  
Vol 22 (1) ◽  
pp. 165-172 ◽  
Author(s):  
A. Barna ◽  
I. B. Földes ◽  
J. Bohus ◽  
S. Szatmári

Abstract An active beam-pointing stabilization system has been developed for a high-power KrF laser system to eliminate the long-term drift of the directional change of the beam in order to have a stable focusing to a high intensity. The control of the beam direction was achieved by a motor-driven mirror activated by an electric signal obtained by monitoring the position of the focus of the output beam. Instead of large sized UV-sensitive position sensitive detectors a simple arrangement with scatter plates and photodiodes are used to measure the directionality of the beam. After the beam stabilization the long-term residual deviation of the laser shots is ~14 μrad, which is comparable to the shot-to-shot variation of the beam (~12 μrad). This deviation is small enough to keep the focal spot size in a micrometer range when tightly focusing the beam using off-axis parabolic mirrors.


Author(s):  
N.G. Basov ◽  
V.G. Bakaev ◽  
G.E. Metreveli ◽  
G.V. Sychugov ◽  
A.D. Vadkovskii ◽  
...  
Keyword(s):  

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