Generation of continuous-wave coherent radiation tunable down to 190.8nm in ?-BaB2O4

1991 ◽  
Vol 53 (1) ◽  
pp. 11-13 ◽  
Author(s):  
M. Watanabe ◽  
K. Hayasaka ◽  
H. Imajo ◽  
J. Umezu ◽  
S. Urabe
Keyword(s):  
Continuous Wave ◽  
Coherent Radiation

All-solid-state light source for generation of tunable continuous-wave coherent radiation near 202 nm

1999 ◽  
Vol 16 (10) ◽  
pp. 1668 ◽  
Author(s):  
Kensuke Matsubara ◽  
Utako Tanaka ◽  
Hidetsuka Imajo ◽  
Masayoshi Watanabe ◽  
Shinji Urabe
Keyword(s):  
Solid State ◽  
Light Source ◽  
Continuous Wave ◽  
Coherent Radiation

High-Power, Continuous-wave, Source Of Coherent Radiation In 2-D Airy Intensity Distribution

2015 ◽  
Author(s):  
A. Aadhi ◽  
Apurv ChaitanyaN. ◽  
M. V. Jabir ◽  
Pravin Vaity ◽  
R. P. Singh ◽  
...  
Keyword(s):  
Intensity Distribution ◽  
High Power ◽  
Continuous Wave ◽  
Coherent Radiation ◽  
Wave Source

Practical Picture Processing

1974 ◽  
Vol 32 ◽  
pp. 338-339
Author(s):  
T. A. Welton
Keyword(s):  
Radiation Damage ◽  
Coherence Length ◽  
Spatial Information ◽  
State Of The Art ◽  
Coherent Radiation ◽  
The State ◽  
Energy Spread ◽  
Electron Micrograph ◽  
Picture Processing ◽  
Molecular Skeleton

Various authors have emphasized the spatial information resident in an electron micrograph taken with adequately coherent radiation. In view of the completion of at least one such instrument, this opportunity is taken to summarize the state of the art of processing such micrographs. We use the usual symbols for the aberration coefficients, and supplement these with £ and 6 for the transverse coherence length and the fractional energy spread respectively. He also assume a weak, biologically interesting sample, with principal interest lying in the molecular skeleton remaining after obvious hydrogen loss and other radiation damage has occurred.

Microstructures of Laser Processed Fe-Cr Surface Alloys

1981 ◽  
Vol 39 ◽  
pp. 328-329
Author(s):  
P. A. Molian ◽  
K. H. Khan ◽  
W. E. Wood
Keyword(s):  
Cooling Rate ◽  
Pure Iron ◽  
Continuous Wave ◽  
Laser Surface ◽  
Material Surface ◽  
Constitution Diagram ◽  
Incident Power ◽  
Surface Alloying ◽  
Laser Surface Alloying ◽  
Spot Diameter

In recent years, the effects of chromium on the transformation characteristics of pure iron and the structures produced thereby have been extensively studied as a function of cooling rate. In this paper, we present TEM observations made on specimens of Fe-10% Cr and Fe-20% Cr alloys produced through laser surface alloying process with an estimated cooling rate of 8.8 x 104°C/sec. These two chromium levels were selected in order to study their phase transformation characteristics which are dissimilar in the two cases as predicted by the constitution diagram. Pure iron (C<0.01%, Si<0.01%, Mn<0.01%, S=0.003%, P=0.008%) was electrodeposited with chromium to the thicknesses of 40 and 70μm and then vacuum degassed at 400°F to remove the hydrogen formed during electroplating. Laser surface alloying of chromium into the iron substrate was then performed employing a continuous wave CO2 laser operated at an incident power of 1200 watts. The laser beam, defocussed to a spot diameter of 0.25mm, scanned the material surface at a rate of 30mm/sec, (70 ipm).

1848: Revolix 70 Watt 2 Micron Continuous Wave Laser Vaporesection of the Prostate. Preliminary Results After a One Year Follow-Up

2007 ◽  
Vol 177 (4S) ◽  
pp. 614-614
Author(s):  
Thorsten Bach ◽  
Thomas R.W. Herrmann ◽  
Roman Ganzer ◽  
Andreas J. Gross
Keyword(s):  
Continuous Wave ◽  
Continuous Wave Laser ◽  
Preliminary Results ◽  
Wave Laser ◽  
One Year
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