1987
DOI: 10.1016/0040-6090(87)90116-7
|View full text |Cite
|
Sign up to set email alerts
|

Temperature dependence of transport properties of evaporated indium tin oxide films

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
10
0

Year Published

1991
1991
2016
2016

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 43 publications
(10 citation statements)
references
References 9 publications
0
10
0
Order By: Relevance
“…From Equation 6 the position of the Fermi level at 300 K can be obtained to yield $ E_{\rm c} - E_{\rm F} = 33.1 {\rm meV}\le 2k_{\rm B} T \approx 51.8 {\rm meV} $ , indicating that the ZnO NW used in this work is a weak degenerate semiconductor. We thus assume that the lattice vibration scattering mobility is inversely proportional to the temperature 20–22. To gain a qualitative understanding, we note that the conduction is mainly contributed by electrons near the Fermi level and the mobility of the electron can be expressed as $ \mu = {{e}\over{{m_{\rm n}^ *}}}{{{\left\langle {\tau v^2} \right\rangle}}\over{{\left\langle {v^2} \right\rangle}}} = {{{e\tau_{\rm F}}}\over{{m_{\rm n}^ *}}} $ , where v is the velocity of the electron, <> denotes statistical average, and $ \tau_{\rm F} $ is the time related to the mean free path for electrons near the Fermi level and is velocity independent.…”
Section: Resultsmentioning
confidence: 99%
“…From Equation 6 the position of the Fermi level at 300 K can be obtained to yield $ E_{\rm c} - E_{\rm F} = 33.1 {\rm meV}\le 2k_{\rm B} T \approx 51.8 {\rm meV} $ , indicating that the ZnO NW used in this work is a weak degenerate semiconductor. We thus assume that the lattice vibration scattering mobility is inversely proportional to the temperature 20–22. To gain a qualitative understanding, we note that the conduction is mainly contributed by electrons near the Fermi level and the mobility of the electron can be expressed as $ \mu = {{e}\over{{m_{\rm n}^ *}}}{{{\left\langle {\tau v^2} \right\rangle}}\over{{\left\langle {v^2} \right\rangle}}} = {{{e\tau_{\rm F}}}\over{{m_{\rm n}^ *}}} $ , where v is the velocity of the electron, <> denotes statistical average, and $ \tau_{\rm F} $ is the time related to the mean free path for electrons near the Fermi level and is velocity independent.…”
Section: Resultsmentioning
confidence: 99%
“…This is anticipated as the crystallite size is significantly larger than the mean free path of our charge carriers, typically a few nm 42 , and at high carrier concentrations changes in the levels of ionised impurity scattering will dominate the charge transport 43 . There is however a change in carrier concentration and charge mobility consistent with the observed changes in preferential orientation at low doping concentrations.…”
Section: Resultsmentioning
confidence: 99%
“…It is clear that n remains constant in a wide T range from liquid-helium temperatures up to 300 K. In the as-deposited sample, the n value approaches ∼ 1 × 10 21 cm −3 . Temperature independent n in the ITO material has been reported by a number of groups [61,[74][75][76].…”
Section: Relevant Electronic Parametersmentioning
confidence: 99%