Influence of Doping Density on the Current−Voltage Characteristics of p-Type Silicon in Dilute Hydrofluoric Acid

2007 ◽  
Vol 112 (1) ◽  
pp. 303-307 ◽  
Author(s):  
T. L. S. L. Wijesinghe ◽  
S. Q. Li ◽  
D. J. Blackwood
Author(s):  
Д.А. Кудряшов ◽  
А.С. Гудовских ◽  
А.А. Максимова ◽  
А.И. Баранов ◽  
А.В. Уваров ◽  
...  

The possibility of evaluation the degree of damage to the near-surface layer of p-type silicon using a selective contact based on MoOx/p-Si is shown. A strong sensitivity of the current-voltage characteristics to the states on the silicon surface formed during the deposition of silicon oxide by magnetron sputtering is demonstrated.


2011 ◽  
Vol 8 (3) ◽  
pp. 784-787
Author(s):  
Ahmed Gharbi ◽  
Boudjemaa Remaki ◽  
Aomar Halimaoui ◽  
Daniel Bensahel ◽  
Abdelkader Souifi

2014 ◽  
Vol 11 (11-12) ◽  
pp. 1697-1702 ◽  
Author(s):  
Tleuzhan Turmagambetov ◽  
Sébastien Dubois ◽  
Jean-Paul Garandet ◽  
Benoit Martel ◽  
Nicolas Enjalbert ◽  
...  

1999 ◽  
Vol 558 ◽  
Author(s):  
T. Matsukawa ◽  
K. Tokunaga ◽  
S. Kanemaru ◽  
J. Itoh

ABSTRACTField emission characteristics from n- and p-type silicon gated emitter tips have been investigated in detail by means of experiments and theoretical estimation of band-bending induced by surface states. Single-tip emitters have been fabricated from n- and p-type silicon and their current-voltage characteristics have been evaluated. The field emission from the p-type emitter has been found to occur at lower extraction voltage than that of the n-type emitter. As the theoretical approach to the origin of the phenomena, potential distribution in the emitter tips has been calculated by using device simulation technique. The surface states of the n-type emitter tip are negatively charged and form a potential barrier against the electrons. On the contrary, there is no potential barrier in the p-type tips. The potential barrier in the n-type tip prevents electrons from reaching the tip apex. This is the reason why the emission current of the n-type emitter was suppressed lower than that of the p-type emitter.


1999 ◽  
Vol 607 ◽  
Author(s):  
S. Kato ◽  
T. Horikoshi ◽  
T. Ohkubo ◽  
T. Iida ◽  
Y. Takano

AbstractThe bulk crystal of silicon germanium was grown by vertical Bridgman method with germanium composition, x, varying from 0.6 to 1.0. The temperature dependent variation of the mobility is indicative of alloy scattering dominantly for the bulk wafer. Phosphorus was diffused in as-grown p-type bulk wafer at 850 °C to form pn-junction, and the diffusion coefficient of phosphorus was evaluated as a function of x. The diffusion behavior of phosphorus in silicon germanium is closely correlated with the germanium self-diffusion with changing x. For specimens with lower content x, P concentration profiles indicated “kink and tail” shape, while it was not observed for higher x. For current-voltage characteristics measurement, an ideality factor was obtained.


1985 ◽  
Vol 132 (2) ◽  
pp. 346-349 ◽  
Author(s):  
Nobuyoshi Koshida ◽  
Masahiro Nagasu ◽  
Takashi Sakusabe ◽  
Yuji Kiuchi

1992 ◽  
Vol 281 ◽  
Author(s):  
C. Piskoti ◽  
B. Mykolajenko ◽  
M. Vaziri

ABSTRACTTo study the formation of ohmic contacts, several metals have been deposited on p-types ZnTe and ZnSe epitaxial layers. The metals were deposited on the layers either by simple evaporation or by electroplating. The current-voltage characteristics associated with each metal contact were measured. The preliminary results of these measurements indicate that electroplating is a better technique for making ohmic contact to these layers.


2006 ◽  
Vol 527-529 ◽  
pp. 1571-1574 ◽  
Author(s):  
Cole W. Litton ◽  
Ya.I. Alivov ◽  
D. Johnstone ◽  
Ümit Özgür ◽  
V. Avrutin ◽  
...  

Heteroepitaxial n-ZnO films have been grown on commercial p-type 6H-SiC substrates by plasma-assisted molecular-beam epitaxy, and n-ZnO/p-SiC heterojunction mesa structures have been fabricated and their photoresponse properties have been studied. Current-voltage characteristics of the structures had a very good rectifying diode-like behavior with a leakage current less than 2 x 10-4 A/cm2 at -10 V, a breakdown voltage greater than 20 V, a forward turn on voltage of ∼5 V, and a forward current of ∼2 A/cm2 at 8 V. Photosensitivity of the diodes, when illuminated from ZnO side, was studied at room temperature and photoresponsivity of as high as 0.045 A/W at -7.5 V reverse bias was observed for photon energies higher than 3.0 eV.


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