2010
DOI: 10.1007/s10853-010-4670-6
|View full text |Cite
|
Sign up to set email alerts
|

Optical properties of PbTe doped with Nd

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2011
2011
2015
2015

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 6 publications
(2 citation statements)
references
References 23 publications
0
2
0
Order By: Relevance
“…With increasing Yb content, the Fermi energy and the free electron density grow until the Fermi level reaches the impurity state level, after which no further increase in the electron density in the conduction band is evident, and the Fermi energy is pinned at DE 1 (low-temperature region) for x ¼ 0.015e0.105. On the other hand, with increasing temperature at 413 Ke423 K, the impurity states lead to sink into the band gap, whereas the narrow width of the density-of-states of resonance states ensures a very strict pinning of the Fermi level relative to the conduction band edge, despite the inevitably non-uniform distribution of impurities and electrically active defects throughout the sample [26,27]. At DE 2 (high-temperature region), ln s intrinsic conduction dominates due to the increase in the mobility of the carriers and the reduction of the trapping state and potential barriers [28].…”
Section: Sem and Fesem Observationmentioning
confidence: 99%
“…With increasing Yb content, the Fermi energy and the free electron density grow until the Fermi level reaches the impurity state level, after which no further increase in the electron density in the conduction band is evident, and the Fermi energy is pinned at DE 1 (low-temperature region) for x ¼ 0.015e0.105. On the other hand, with increasing temperature at 413 Ke423 K, the impurity states lead to sink into the band gap, whereas the narrow width of the density-of-states of resonance states ensures a very strict pinning of the Fermi level relative to the conduction band edge, despite the inevitably non-uniform distribution of impurities and electrically active defects throughout the sample [26,27]. At DE 2 (high-temperature region), ln s intrinsic conduction dominates due to the increase in the mobility of the carriers and the reduction of the trapping state and potential barriers [28].…”
Section: Sem and Fesem Observationmentioning
confidence: 99%
“…ZT is given by ZT = S 2 T/rk, where S, r, T, and k are the Seebeck coefficient, electrical resistivity, absolute temperature, and thermal conductivity, respectively [8][9][10]. Therefore, it is necessary to maximize the value of ZT in order to large Seebeck coefficient, low electrical resistivity, and low thermal conductivity of the PbTe material [11].…”
Section: Introductionmentioning
confidence: 99%