Ion Profiling of Implanted Dopants in Si (001) with Excess Vacancy Concentration

Author(s):  
M. Dalponte ◽  
H. Boudinov ◽  
L. V. Goncharova ◽  
T. Feng ◽  
E. Garfunkel ◽  
...  
2009 ◽  
Vol 42 (16) ◽  
pp. 165106
Author(s):  
M Dalponte ◽  
M C Adam ◽  
H I Boudinov ◽  
L V Goncharova ◽  
T Feng ◽  
...  

1963 ◽  
Vol 7 ◽  
pp. 146-158
Author(s):  
J. K. Howard ◽  
D. P. Miller

AbstractHelical dislocations and vacancy aggregates have been reported in lithiumdoped germanium and in diffused silicon. In the present study, defects related to an excess vacancy concentration are examined in as-grown silicon. X-ray topography, etch techniques, and Hall effect are used in determining the conditions of formation of these imperfections. Two distinct types of defects are observed: (1) helical dislocations and (2) dislocation loops. The helical dislocations are identified in the X-ray topographs and correlated to their etch figures. The diameters of the helices in various crystals range from less than 10 to 100 μ. The largest concentration of helices are observed in the initial growth, but prismatic loops or helical segments are also present in the low dislocation density regions of some crystals. The dislocation loop image consists of a pair of opposed arcs. The lengths of images vary from 30 to 400 μ, and the axis of the loop is usually parallel to <110> linage contrast changes with changes in sample orientation, but conclusive Burgers vector determinations are incomplete.The formation of these defects is shown to be directly related to the heat treatment during crystal growth. The total acquisition of vacancies during growth is quite high and is attributed to the “orbital” growth process. In the “orbital” method, the seed check rotates 8-9 rpm about the center of the crucible as the growing crystal rotates 50-60 rpm. A linear relationship exists at room temperature between the vacancy concentration and the antimony impurity concentration. Impurity concentrations were determined independently by chemical and mass spectrograph techniques. A defect complex involving V− and Sb+ in thermal equilibrium is employed to explain this effect.


1983 ◽  
Vol 28 ◽  
Author(s):  
J.V. Wood

ABSTRACTRibbons of a Cu-Al-Ni shape memory alloy have been rapidly solidified by planar flow casting. Attempts have been made to vary casting and secondary quench conditions in order to identify the predominant process variable in determining the subsequent β1↔γ1′ transformation temperatures. By varying wheel speed, wheel material and secondary quenching rate it is concluded that the large excess vacancy concentration has most influence on the as cast ribbon, but that after subsequent heat treatment, the grain size dominates.


1994 ◽  
Vol 354 ◽  
Author(s):  
H.G. Robinson ◽  
C.C. Lee ◽  
T.E. Haynes ◽  
E.L. Allen ◽  
M.D. Deal ◽  
...  

AbstractExperimental observations of dopant diffusion and defect formation are reported as a function of ion energy and implant temperature in Si implanted GaAs. In higher energy implants (>100 keV), little or no diffusion occurs, while at energies less than 100 keV, the amount of dopant redistribution is inversely proportional to energy. The extended defect density shows the opposite trend, increasing with increasing ion energy. Similarly, the diffusion of Si during post implant annealing decreases by a factor of 2.5 as the implant temperature increases from -2 to 40°C. In this same temperature range, the maximum depth and density of extrinsic dislocation loops increases by factors of 3 and 4, respectively. Rutherford Backscattering (RBS) channeling measurements indicate that Si implanted GaAs undergoes an amorphous to crystalline transition at Si implant temperatures between -51 and 40°C. A unified explanation of the effects of ion energy and implant temperature on both diffusion and dislocation formation is proposed based on the known differences in sputter yields between low and high energy ions and crystalline and amorphous semiconductors. The model assumes that the sputter yield is enhanced at low implant energies and by amorphization, thus increasing the excess vacancy concentration. Estimates of excess vacancy concentration are obtained by simulations of the diffusion profiles and are quantitatively consistent with a realistic sputter yield enhancement. Removal of the vacancy rich surface by etching prior to annealing completely suppresses the Si diffusion and increases the dislocation density, lending further experimental support to the model.


2019 ◽  
Author(s):  
Till Fuchs ◽  
Sean Culver ◽  
Paul Till ◽  
Wolfgang Zeier

<p>The sodium-ion conducting family of Na<sub>3</sub><i>Pn</i>S<sub>4</sub>, with <i>Pn</i> = P, Sb, have gained interest for the use in solid-state batteries due to their high ionic conductivity. However, significant improvements to the conductivity have been hampered by the lack of aliovalent dopants that can introduce vacancies into the structure. Inspired by the need for vacancy introduction into Na<sub>3</sub><i>Pn</i>S<sub>4</sub>, the solid solutions with WS<sub>4</sub><sup>2-</sup> introduction are explored. The influence of the substitution with WS<sub>4</sub><sup>2-</sup> for PS<sub>4</sub><sup>3-</sup> and SbS<sub>4</sub><sup>3-</sup>, respectively, is monitored using a combination of X-ray diffraction, Raman and impedance spectroscopy. With increasing vacancy concentration improvements resulting in a very high ionic conductivity of 13 ± 3 mS·cm<sup>-1</sup> for Na<sub>2.9</sub>P<sub>0.9</sub>W<sub>0.1</sub>S<sub>4</sub> and 41 ± 8 mS·cm<sup>-1</sup> for Na<sub>2.9</sub>Sb<sub>0.9</sub>W<sub>0.1</sub>S<sub>4</sub> can be observed. This work acts as a stepping-stone towards further engineering of ionic conductors using vacancy-injection via aliovalent substituents.</p>


2019 ◽  
Author(s):  
Till Fuchs ◽  
Sean Culver ◽  
Paul Till ◽  
Wolfgang Zeier

<p>The sodium-ion conducting family of Na<sub>3</sub><i>Pn</i>S<sub>4</sub>, with <i>Pn</i> = P, Sb, have gained interest for the use in solid-state batteries due to their high ionic conductivity. However, significant improvements to the conductivity have been hampered by the lack of aliovalent dopants that can introduce vacancies into the structure. Inspired by the need for vacancy introduction into Na<sub>3</sub><i>Pn</i>S<sub>4</sub>, the solid solutions with WS<sub>4</sub><sup>2-</sup> introduction are explored. The influence of the substitution with WS<sub>4</sub><sup>2-</sup> for PS<sub>4</sub><sup>3-</sup> and SbS<sub>4</sub><sup>3-</sup>, respectively, is monitored using a combination of X-ray diffraction, Raman and impedance spectroscopy. With increasing vacancy concentration improvements resulting in a very high ionic conductivity of 13 ± 3 mS·cm<sup>-1</sup> for Na<sub>2.9</sub>P<sub>0.9</sub>W<sub>0.1</sub>S<sub>4</sub> and 41 ± 8 mS·cm<sup>-1</sup> for Na<sub>2.9</sub>Sb<sub>0.9</sub>W<sub>0.1</sub>S<sub>4</sub> can be observed. This work acts as a stepping-stone towards further engineering of ionic conductors using vacancy-injection via aliovalent substituents.</p>


1981 ◽  
Vol 24 (4) ◽  
pp. 338-342
Author(s):  
V. A. Klimenko ◽  
S. I. Masharov ◽  
A. F. Rybalko ◽  
N. M. Rybalko ◽  
N. I. Timofeev

Pramana ◽  
2021 ◽  
Vol 95 (3) ◽  
Author(s):  
Monika Goyal ◽  
Vishal Goyal

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