1977
DOI: 10.1051/rphysap:01977001202016700
|View full text |Cite
|
Sign up to set email alerts
|

The physical properties of cadmium telluride

Abstract: 2014 Cet article passe en revue les propriétés structurales, thermiques, mécaniques, optiques et électriques du tellurure de cadmium. Celles-ci sont par ailleurs comparées aux propriétés physiques des autres composés IIB-VIA.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

2
31
1
2

Year Published

1978
1978
2012
2012

Publication Types

Select...
7
1
1

Relationship

0
9

Authors

Journals

citations
Cited by 106 publications
(36 citation statements)
references
References 64 publications
2
31
1
2
Order By: Relevance
“…The choice of CdTe has been motivated by the fact that this semiconductor material allows for a high degree of compensation [12], thus presenting the desired semiinsulating property. Moreover, it displays linear velocityfield characteristics up to several kV=cm at room temperature [12], thus allowing one to apply considerable high voltages without the presence of hot-electron effects. Furthermore, the use of metal-semiconductor contacts is motivated by the fact that metals on semi-insulating materials exhibit the required nearly perfect Ohmic behavior in a wide range of voltages, since the carrier density at the interface imposed by the contact is of the same order of magnitude as the free carrier density of the semi-insulating material [13].…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…The choice of CdTe has been motivated by the fact that this semiconductor material allows for a high degree of compensation [12], thus presenting the desired semiinsulating property. Moreover, it displays linear velocityfield characteristics up to several kV=cm at room temperature [12], thus allowing one to apply considerable high voltages without the presence of hot-electron effects. Furthermore, the use of metal-semiconductor contacts is motivated by the fact that metals on semi-insulating materials exhibit the required nearly perfect Ohmic behavior in a wide range of voltages, since the carrier density at the interface imposed by the contact is of the same order of magnitude as the free carrier density of the semi-insulating material [13].…”
mentioning
confidence: 99%
“…A best fit to the experiments gives a resistance R 323K 0:233 G, which implies a resistivity 0:233 G cm. From these parameters, and by using [12] r 12, the dielectric relaxation time for the material is d 0:3 ms. Therefore, by extracting a mobility corresponding to holes 50 cm 2 =V s from the measurement of the cutoff frequency in the noise spectra in the shot noise region [14] (the sample is known to be p type [15]), and for an applied bias of 10 V, the transit time is T 0:08 ms, thus making accessible the shot noise condition ( T d ) for applied bias above a few tens of volts.…”
mentioning
confidence: 99%
“…As shown in Fig. 2(a), the PL peak energy of the superlattice is smaller than the bandgap energy of either CdTe (1.61 eV) 9,12,13 or cubic CdSe (1.76 eV), 9,10 suggesting a type-II band edge alignment. Furthermore, the PL peak shifts to higher energy as the excess carrier concentration increases.…”
Section: à3mentioning
confidence: 91%
“…A second advantage in controlling the carrier density in p-CdTe is in the optimization of the open-circuit voltage, V, , (5). Group V elements P, As, or Sb are readily incorporated into single crystals of CdTe grown from the liquid (6), with the carrier density reaching a maximum of -2~1 0 '~ using P (7). On the other hand, preparation of p-CdTe from the vapor by conventional film growth techniques has been difficult.…”
Section: Introductionmentioning
confidence: 99%