Studies of Laser Annealed GaAs (100), (110) and (111) Surfaces

1981 ◽  
Vol 4 ◽  
Author(s):  
D. M. Zehner ◽  
C. W. White ◽  
B. R. Appleton ◽  
G. W. Ownby

ABSTRACTThe surface regions of (100), (110) and (111) oriented single crystals of GaAs have been investigated by the combine techniques of LEED, AES and RBS subsequent to their irradiation in UHV with the output of a Q–switched, ruby laser (0.15−0.8 J/cm2, 15 × 10−9 sec). Clean surfaces, as determined by AES, were obtained after Ar+ sputtering followed by laser irradiation. LEED observations indicate that the degree of disorder in the outermost surface layers remaining after irradiation depends on the crystal orientation. Although the relative intensities of Ga and As Auger transitions in spectra obtained from sputtered and laser annealed surfaces are similar, the differences in lineshape in these spectra of the M2,3M4,5M4,5 Ga Auger transition indicate that in the laser annealed case there are local regions which are nonstoichiometric. These observations are confirmed by RBS results, and this technique has been used to determine the stoichiometry and to characterize the damage in the subsurface region for all orientations.

1983 ◽  
Vol 23 ◽  
Author(s):  
S. U. Campisano ◽  
D. C. Jacobson ◽  
J. M. Poate ◽  
A. G. Cullis ◽  
N. G. Chew

ABSTRACTThe formation of amorphous Si by the quench of a thin surface layer melted by fast UV laser irradiation has been investigated. The starting (111) surface layers were either pure or doped with As, Bi, In and Te by implantation. The asimplanted samples were recrystallized by ruby laser irradiation resulting in surface accumulation of Bi,In and Te. For the same UV irradiation condition, the amorphous layer formed in As, Bi, In or Te doped Si is about twice the thickness of the amorphous layer formed on pure Si. In the presence of the surface accumulation of Bi, In or Te, the amorphization results in an inward segregation of the dopant. For In, a very thin metal layer ˜15Å thick, is formed 150Å beneath the amorphous surface. These results show that the amorphous-liquid interfacial segregation coefficients for Bi, In or Te are less than unity and that the amorphous solidification proceeds from the surface and bottom of the liquid layer.


1982 ◽  
Vol 13 ◽  
Author(s):  
D. M. Zehner ◽  
C. W. White

ABSTRACTThe surface regions of semiconductor single crystals have been examined following laserannealing in an ultrahigh vacuum environment with the output of a pulsed ruby laser. Atomically clean surfaces with impurity levels below 0.1% of a monolayer can be produced by multiple pulse irradiation. Ordered surface structures are produced on low index oriented crystals as well as crystals slightly misoriented. Metastable surface structures exhibiting (l×1) LEED patterns have been produced on (111) orientations and are believed to be a consequence of the rapid cooling rates of 109 degs/sec achieved with the laser irradiation process. The surface and subsurface regions of ion-implanted Si crystals have been examined both before and after laser irradiation and results obtained from Si samples implanted with As are discussed.


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.


1979 ◽  
Vol 30 (3) ◽  
pp. 369-372
Author(s):  
M. V. Vasilenko ◽  
G. V. Bukin ◽  
F. F. Gavrilov ◽  
A. V. Kruzhalov ◽  
V. N. Mizgulin ◽  
...  

1980 ◽  
Vol 37 (4) ◽  
pp. 385-387 ◽  
Author(s):  
L. Buene ◽  
J. M. Poate ◽  
D. C. Jacobson ◽  
C. W. Draper ◽  
J. K. Hirvonen

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