Lattice Temperature of GaAs and Si During Nanosecond Laser Annealing

1983 ◽  
Vol 23 ◽  
Author(s):  
A. Pospieszczyk ◽  
M. Abdel Harith ◽  
B. Stritzker

ABSTRACTSingle crystals of GaAs (100) and Si (110) were laser annealed with a 20 ns ruby laser pulse. Both the velocity distribution and the density variation of evaporated Ga or As and Si atoms were determined by a time-of-flight measurement. In addition time-resolved measurements were made of the reflectivity of the surface during the laser annealing. The data consistently show that the molten phase occurs at energy densities of ≳ 0.35 J cm–2 for GaAs and ≳O.8 J cm for Si.

1980 ◽  
Vol 1 ◽  
Author(s):  
Nobuyoshi Natsuaki ◽  
Takao Miyazaki ◽  
Makoto Ohkura ◽  
Toru Nakamura ◽  
Masao Tamura ◽  
...  

ABSTRACTBipolar transistors with laser annealed base and emitter, as well as those with furnace annealed base and laser annealed emitter, have been successfully fabricated using Q-switched ruby laser pulse irradiation. The performance of laser asannealed transistors is rather poor. However, it can be improved, to some extent, by relatively low temperature furnace annealing after laser irradiation. DC and RF characteristics of laser annealed transistors are presented in conjunction with laser irradiation effects on the characteristics of conventionally fabricated transistors.


1985 ◽  
Vol 51 ◽  
Author(s):  
W. Pamler ◽  
E. E. Marinero ◽  
M. Chen ◽  
V. B. Jipson

ABSTRACTWe report on the growth and redistribution of Au clusters caused by nanosecond laser interaction of Aux(TeO2 )1−x thin films with intense excimer laser radiation. This laser-induced phenomenon is studied in a time-resolved manner using transient reflectivity and transmissivity techniques. Structural and compositional changes are investigated using Rutherford Backscattering, XPS depth profiling, x-ray diffraction and conductivity measurements. Our studies indicate that melting of the binary structure initializes segregation, growth and coalescence of Au crystallites in the amorphous TeO2 matrix.


1999 ◽  
Vol 68 (6) ◽  
pp. 637-641 ◽  
Author(s):  
J. Jersch ◽  
F. Demming ◽  
I. Fedotov ◽  
K. Dickmann

1998 ◽  
Vol 66 (6) ◽  
pp. 615-619 ◽  
Author(s):  
J. Boneberg ◽  
M. Tresp ◽  
M. Ochmann ◽  
H.-J. Münzer ◽  
P. Leiderer

1981 ◽  
Vol 4 ◽  
Author(s):  
R. T. Williams ◽  
M. N. Kabler ◽  
J. P. Long ◽  
J. C. Rife ◽  
T. R. Royt

ABSTRACTSpectra of photoelectrons and thermionic electrons emitted from silicon during pulsed laser irradiation at energy densities encompassing the thresholds for laser annealing and damage are reported. Annealing is accomplished with a 90-nsec pulse of 532-nm light, which may be accompanied by a 266-nm probe pulse. A cylindrical mirror analyzer is used for energy resolution of emitted electrons. Time-resolved reflectivity at 633 nm verifies attainment of the high-reflectivity annealing phase. Spectral widths and total yields imply a modest electron temperature (T < 3000 K) during annealing. The data suggest that the work function of the silicon (111) face may increase about 0.6 eV upon transition to the molten phase.


Author(s):  
Siyuan Geng ◽  
Zhifeng Yao ◽  
Qiang Zhong ◽  
Yuxin Du ◽  
Ruofu Xiao ◽  
...  

Abstract The objective of this paper is to reveal the attenuation characteristics of a shock wave after optical breakdown in water, with laser pulses of 10-ns duration. A high time-resolved shadowgraph method is applied to capture the temporal evolutions of the cavitation bubble wall and shock wave. The experiments are carried out on a single bubble generated far away from the free surface and the rigid walls with laser pulse energies of 22 mJ, 45 mJ and 60 mJ. The results show that a high, time-resolved, wave front velocity of the shock wave is identified, and the maximum velocity can reach up to around 4000 m/s. An asymmetric shock wave is observed at the very start of the bubble expansion stage, and the process of the sharp attenuation of wave front velocity down to sound velocity, is accomplished within 310-ns. The possible relationship of the cavitation bubble and the shock wave is discussed and a prediction model, using the maximum bubble radius and the corresponding time calculated by the Gilmore model, is proposed to calculate the location of the wave front.


Author(s):  
Yibo Gao ◽  
Yun Zhou ◽  
Benxin Wu ◽  
Sha Tao ◽  
Ronald L. Jacobsen ◽  
...  

Silicon carbide, due to its unique properties, has many promising applications in optics, electronics, and other areas. However, it is difficult to micromachine using mechanical approaches due to its brittleness and high hardness. Laser ablation can potentially provide a good solution for silicon carbide micromachining. However, previous studies of silicon carbide ablation by nanosecond laser pulses at infrared wavelengths are very limited on material removal mechanism, and the mechanism has not been well understood. In this paper, experimental study is performed for silicon carbide ablation by 1064 nm and 200 ns laser pulses through both nanosecond time-resolved in situ observation and laser-ablated workpiece characterization. This study shows that the material removal mechanism is surface vaporization, followed by liquid ejection (which becomes clearly observable at around 1 μs after the laser pulse starts). It has been found that the liquid ejection is very unlikely due to phase explosion. This study also shows that the radiation intensity of laser-induced plasma during silicon carbide ablation does not have a uniform spatial distribution, and the distribution also changes very obviously when the laser pulse ends.


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