2013
DOI: 10.1134/s1063783413070342
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Study of the charge carrier transport through a metal-poly(arylenephthalide)-class polymer interface

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Cited by 12 publications
(3 citation statements)
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“…For non-conjugated polymers, this level is often located in the middle of the gap between the upper occupied orbital and the lower vacant one. The experimental measurement of the height of the potential barrier confirmed the validity of this statement [61]. It should be noted that the inexplicably underestimated height of the potential barrier [62] in a structure with a polymer boundary had been repeatedly noted previously, corresponding to the value determined according to Equation (2).…”
Section: Influence Of the Electrode Materialssupporting
confidence: 78%
“…For non-conjugated polymers, this level is often located in the middle of the gap between the upper occupied orbital and the lower vacant one. The experimental measurement of the height of the potential barrier confirmed the validity of this statement [61]. It should be noted that the inexplicably underestimated height of the potential barrier [62] in a structure with a polymer boundary had been repeatedly noted previously, corresponding to the value determined according to Equation (2).…”
Section: Influence Of the Electrode Materialssupporting
confidence: 78%
“…The role of lateral fragments of molecule (containing the paramagnetic oxygen) for the electron transport in polymer film have just been emphasized [7]. The explanation that the magnetic field initiates the liberation of trapped electrons is confirmed by the fact that the CVC for decreasing bias voltage are disposed higher, than ones for the increasing bias voltage.…”
Section: Resultsmentioning
confidence: 96%
“…Для анализа влияния изменения параметров контакта на границе In/полимер на транспорт носителей заряда была проведена оценка высоты потенциального барьера для электронов в зависимости от концентрации допанта. Ранее в работах [25][26][27] было показано, что преобладающим механизмом переноса заряда в структуре металл−ПДФ−металл при комнатных температурах и аналогичных полях является термоэлектронная эмиссия Шоттки. В этом случае плотность тока термоэлектронной эмиссии с учетом понижения барьера за счет приложенного внешнего поля задается уравнением (5):…”
Section: объекты и методы исследованияunclassified