Effect of the Distance from the Focusing Lens to the Target Surface on the Infrared Spectrum

2020 ◽  
Vol 10 (01) ◽  
pp. 85-90
Author(s):  
彦明 马
1977 ◽  
Vol 32 (10) ◽  
pp. 1100-1107 ◽  
Author(s):  
R. P. Godwin ◽  
C. G. M. van Kessel ◽  
J. N. Olsen ◽  
P. Sachsenmaier ◽  
R. Sigel ◽  
...  

Optical calorimetry of laser radiation reflected from plane targets irradiated by a 0.3 J/30 ps Nd-laser pulse (λ = 1.06 μm) has been performed. A 2π-ellipsoidal mirror was used for scattered light collection. We find that scattering outside the solid angle of the focusing lens is a major reflection loss from the target. A maximum fraction of 0.5 of the incident pulse energy was absorbed in the target with only a very weak dependence on pulse energy and target material. We emphasize that measurements made with sharp focusing on the target surface are difficult to compare with theoretical models in the plane wave/plane target approximation


2008 ◽  
Vol 26 (2) ◽  
pp. 189-196 ◽  
Author(s):  
A. Kasperczuk ◽  
T. Pisarczyk ◽  
M. Kalal ◽  
M. Martinkova ◽  
J. Ullschmied ◽  
...  

AbstractThis paper is devoted to investigations of laser energy transfer into solid targets with respect to the focusing lens focal point position relative to the solid target surface as obtained at the PALS laser facility. The third harmonic of the PALS laser beam with energy ~90 J and pulse duration ~250 ps (FWHM) was used for irradiation of two kinds of targets made of Cu: a slab and a 3.6 µm thick foil. The focal point of the beam was located either inside or in front of the target surface, and care was taken to ensure the same laser spot radii in both cases (250 µm). It was demonstrated that these two opposite focal point positions give rise to significantly different laser-plasma interactions: with either depression or maximum of the laser intensity distribution in the center of the beam, respectively. It was also verified that the focal point position inside of the target is favorable for plasma jets creation, whereas the opposite case is more effective for acceleration of flyers.


2019 ◽  
Vol 34 (5) ◽  
pp. 1018-1025 ◽  
Author(s):  
Wanpeng Xu ◽  
Anmin Chen ◽  
Qiuyun Wang ◽  
Dan Zhang ◽  
Ying Wang ◽  
...  

This paper exhibits the generation of high-temperature and low-density plasma with strong spectral intensity by changing the distance between focusing lens and target surface in femtosecond laser-induced breakdown spectroscopy.


2018 ◽  
Vol 25 (3) ◽  
pp. 033302 ◽  
Author(s):  
Ying Wang ◽  
Anmin Chen ◽  
Qiuyun Wang ◽  
Laizhi Sui ◽  
Da Ke ◽  
...  

Author(s):  
T.S. Savage ◽  
R. Ai ◽  
D. Dunn ◽  
L.D. Marks

The use of lasers for surface annealing, heating and/or damage has become a routine practice in the study of materials. Lasers have been closely looked at as an annealing technique for silicon and other semiconductors. They allow for local heating from a beam which can be focused and tuned to different wavelengths for specific tasks. Pulsed dye lasers allow for short, quick bursts which can allow the sample to be rapidly heated and quenched. This short, rapid heating period may be important for cases where diffusion of impurities or dopants may not be desirable.At Northwestern University, a Candela SLL - 250 pulsed dye laser, with a maximum power of 1 Joule/pulse over 350 - 400 nanoseconds, has been set up in conjunction with a Hitachi UHV-H9000 transmission electron microscope. The laser beam is introduced into the surface science chamber through a series of mirrors, a focusing lens and a six inch quartz window.


Author(s):  
W. Brünger

Reconstructive tomography is a new technique in diagnostic radiology for imaging cross-sectional planes of the human body /1/. A collimated beam of X-rays is scanned through a thin slice of the body and the transmitted intensity is recorded by a detector giving a linear shadow graph or projection (see fig. 1). Many of these projections at different angles are used to reconstruct the body-layer, usually with the aid of a computer. The picture element size of present tomographic scanners is approximately 1.1 mm2.Micro tomography can be realized using the very fine X-ray source generated by the focused electron beam of a scanning electron microscope (see fig. 2). The translation of the X-ray source is done by a line scan of the electron beam on a polished target surface /2/. Projections at different angles are produced by rotating the object.During the registration of a single scan the electron beam is deflected in one direction only, while both deflections are operating in the display tube.


1996 ◽  
Vol 89 (4) ◽  
pp. 1145-1155
Author(s):  
JACQUES WALRAND ◽  
GHISLAIN BLANQUET ◽  
JEAN-FRANCOIS BLAVIER ◽  
HARALD BREDOHL ◽  
IWAN DUBOIS

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