2016
DOI: 10.1016/j.tsf.2016.07.073
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Surface pattering of Ge–As–Se thin films by electric charge accumulation

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Cited by 15 publications
(15 citation statements)
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“…It can be seen that for G < 2400 mC•cm −2 the height of the surface relief gradually grows to 100-125 nm and for G > 2400 mC•cm −2 , relief height decreases. The changing of shape and parameters of the obtained surface relief on As3S77Ge20 film can be explained by the charge model, which was used earlier for the relief formation processes in Ge-As-Se chalcogenide films [5,6,11]. The formation of surface relief is due to structural changes in the film and the emergence of a space charge region (SCR) during the interaction of the film and the electron beam.…”
Section: Resultsmentioning
confidence: 95%
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“…It can be seen that for G < 2400 mC•cm −2 the height of the surface relief gradually grows to 100-125 nm and for G > 2400 mC•cm −2 , relief height decreases. The changing of shape and parameters of the obtained surface relief on As3S77Ge20 film can be explained by the charge model, which was used earlier for the relief formation processes in Ge-As-Se chalcogenide films [5,6,11]. The formation of surface relief is due to structural changes in the film and the emergence of a space charge region (SCR) during the interaction of the film and the electron beam.…”
Section: Resultsmentioning
confidence: 95%
“…The formation of surface relief is due to structural changes in the film and the emergence of a space charge region (SCR) during the interaction of the film and the electron beam. The penetration of primary electrons into the film leads to the accumulation of charge in the film and on its surface, as well as the emission of electrons from the film back into the vacuum [6].…”
Section: Resultsmentioning
confidence: 99%
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“…Однак, дослідження впливу електронного опромінення на халькогенідні плівки показали на наявність модифікації їх поверхні електронним променем [3][4][5] Зростання дози опромінення понад 9.310 4 мкКл/см 2 (t>5 мс) приводить до інверсії форми електронно індукованого рельєфу. В області доз 9.310 4 до 9.310 6 мкКл/см 2 при електронному опроміненні на поверхні плівки утворюються кратери з профілем гаусового типу.…”
Section: вступunclassified
“…Як було показано в [5], процес формування поверхневого рельєфу в халькогенідних плівках визначається як параметрами електронного променя так і товщиною та електрофізичними властивостями плівки.…”
Section: вступunclassified