1958
DOI: 10.1103/physrev.109.601
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High-Voltage Photovoltaic Effect

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Cited by 69 publications
(16 citation statements)
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“…The exact shape and dimensions of the space charge layer depend on a number of factors that are material and in some cases sample specific. It has been shown that photo deposition of silver can occur on both positive and negative domains on PZT when it is [100] orientated, but that silver only deposits on PZT [111] when it is positively charged [74]. This is due to variations in the density of states and also in the variation in the remnant polarisation of the sample, which impacts the shape of the space charge layer and screening processes.…”
Section: Electrostatic Properties Of the Ferroelectric Surfacementioning
confidence: 99%
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“…The exact shape and dimensions of the space charge layer depend on a number of factors that are material and in some cases sample specific. It has been shown that photo deposition of silver can occur on both positive and negative domains on PZT when it is [100] orientated, but that silver only deposits on PZT [111] when it is positively charged [74]. This is due to variations in the density of states and also in the variation in the remnant polarisation of the sample, which impacts the shape of the space charge layer and screening processes.…”
Section: Electrostatic Properties Of the Ferroelectric Surfacementioning
confidence: 99%
“…A mechanism, based on similar behaviour observed in semiconductor materials such as thin polycrystalline semiconductor films of Cadmium telluride [111] and striated zinc sulphide crystals [112], where the potential differences across individual crystallites, having the same origins as single crystal surface barrier layers, create multiple smaller than band gap voltages that add up in series across the whole was proposed, in 1975, by Brody and Crowne [89] with the total voltage written as:…”
Section: Ferroelectric Photocurrents and The Anomalously High Photovomentioning
confidence: 99%
“…Аномальный фотовольтаический эффект (АФЭ) в тонких пленках полупроводников известен с се-редины прошлого века [1]. В силу определенных факторов -относительно низкого коэффициента полез-ного действия процесса преобразования энергии оптического излучения в электрическое, высокого внут-реннего сопротивления и др.…”
Section: Introductionunclassified
“…Электрический отклик при воздействии лазерного излучения видимого диапазона наблюдался ра-нее в различных аморфных тонких пленках: CdTe [1,4,5], германия [6], платины и палладия [7], молиб-дена и вольфрама [8]. Для описания эффекта возникновения разности потенциалов при воздействии ла-зерного излучения был предложен ряд моделей, объясняющих наблюдаемое явление с помощью множе-ства p-n-переходов, обусловленных неоднородностями пленки [1,4], нормальным и аномальным эффек-том Дембера [6], а также, в случае металлических пленок, возникновением микроскопических термопар на границах зерен и эффекта Зеебека [7,8].…”
Section: Introductionunclassified
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