Correlation of Surface Photovoltaic Technique with Deep Level Transient Spectroscopy for Iron Concentration Measurement in P‐Type Silicon Wafers

1991 ◽  
Vol 138 (5) ◽  
pp. 1424-1426 ◽  
Author(s):  
K. Ryoo ◽  
W. E. Socha
2012 ◽  
Vol 9 (10-11) ◽  
pp. 1992-1995 ◽  
Author(s):  
C. K. Tang ◽  
L. Vines ◽  
B. G. Svensson ◽  
E. V. Monakhov

2016 ◽  
Vol 254 (4) ◽  
pp. 1600593
Author(s):  
Eddy Simoen ◽  
Suseendran Jayachandran ◽  
Annelies Delabie ◽  
Matty Caymax ◽  
Marc Heyns

2002 ◽  
Vol 719 ◽  
Author(s):  
Yutaka Tokuda ◽  
Hiroyuki Iwata

AbstractHydrogen implantation has been used to anneal defects produced in p-type silicon by boron implantation. Boron implantation is performed with an energy of 300 keV to a dose of 1×109 cm-2. Deep level transient spectroscopy measurements show the production of four hole traps (Ev + 0.21, 0.35, 0.50, 0.55 eV) by boron implantation. Subsequent hydrogen implantation is performed with energies of 60, 90, 120 and 150 keV to a dose of 2×1010 cm-2. Among four traps produced by boron implantation, the most significant effect of hydrogen implantation is observed on one trap (Ev + 0.50 eV). A 62% decrease in concentration is caused for this trap by hydrogen implantation with energies of 120 and 150 keV. This partial annealing is ascribed to the reaction of boron-implantation-induced defects with point defects produced by hydrogen implantation.


2005 ◽  
Vol 108-109 ◽  
pp. 279-284 ◽  
Author(s):  
O.F. Vyvenko ◽  
N.V. Bazlov ◽  
M.V. Trushin ◽  
A.A. Nadolinski ◽  
Michael Seibt ◽  
...  

Influence of annealing in molecular hydrogen as well as of treatment in hydrogen plasma (hydrogenation) on the electrical properties of NiSi2 precipitates in n- and p-type silicon has been studied by means of deep level transient spectroscopy (DLTS). Both annealing and hydrogenation gave rise to noticeable changes of the shape of the DLTS-peak and of the character of its dependence on the refilling pulse duration that according to [1] allows one to classify the electronic states of extended defects as “band-like” or “localized”. In both n- and p-type samples DLTS-peak in the initial as quenched samples showed bandlike behaviour. Annealing or hydrogenation of n-type samples converted the band-like states to the localised ones but differently shifted the DLTS-peak to higher temperatures. In p-type samples, the initial “band-like” behaviour of DLTS peak remained qualitatively unchanged after annealing or hydrogenation. A decrease of the DLTS-peak due to precipitates and the appearance of the peaks due to substitutional nickel and its complexes were found in hydrogenated p-type sample after removal of a surface layer of 10-20µm.


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