RU2011141984A - METHOD FOR TESTING CMOS / KND SEMICONDUCTOR BIS ON THE RESISTANCE TO EFFECTS OF SINGLE FAILURES FROM EXPOSURE TO HEAVY CHARGED SPACE PARTICLES - Google Patents
METHOD FOR TESTING CMOS / KND SEMICONDUCTOR BIS ON THE RESISTANCE TO EFFECTS OF SINGLE FAILURES FROM EXPOSURE TO HEAVY CHARGED SPACE PARTICLES Download PDFInfo
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- RU2011141984A RU2011141984A RU2011141984/28A RU2011141984A RU2011141984A RU 2011141984 A RU2011141984 A RU 2011141984A RU 2011141984/28 A RU2011141984/28 A RU 2011141984/28A RU 2011141984 A RU2011141984 A RU 2011141984A RU 2011141984 A RU2011141984 A RU 2011141984A
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Abstract
1. Способ испытаний полупроводниковых БИС технологии КМОП/КНД на стойкость к эффектам единичных сбоев от воздействия тяжелых заряженных частиц (ТЗЧ) космического пространства путем облучения ограниченной выборки БИС импульсным гамма-нейтронным ионизирующим излучением ядерного реактора или импульсным рентгеновским излучением электрофизических установок (ЭФУ) с эквивалентной дозой, вызывающей равную с ТЗЧ генерацию радиационно-индуцированного заряда в чувствительном объеме БИС, отличающийся тем, что вместо независимого облучения гамма-нейтронным излучением реактора, а также протонами, электронами и ТЗЧ, производят облучение только гамма-нейтронным излучением импульсного ядерного реактора (ИЯР) со средней энергией 1,0-3,0 МэВ или импульсным рентгеновским излучением ЭФУ и для определения стойкости к воздействию ТЗЧ с величиной порогового значения линейных потерь энергии LETв диапазоне от единиц до сотни МэВ·см/г используют значение коэффициента относительной эффективности RDEF (Relative Dose Enhancement Factor) воздействия полной поглощенной дозы рентгеновского или гамма-излучения по отношению к величине LETс использованием соотношенияв единицахгде ρ - плотность облучаемого полупроводникового материала, г·см;- максимальное значение хорды в чипе структуры МДП, см; a - ширина чипа структуры МДП, см; b - длина чипа, см; c - высота чипа; см;- константа радиационной генерации носителей заряда, Кл·смрад(M);- предельное значение доли нерекомбинированного радиационно-индуцированного заряда в структуре МДП при воздействии излучения моделирующей установки (МУ) в присутствии приложенного электрического поля напряженностью E, МВ·см;- ф�1. Method for testing semiconductor LSI CMOS / KND technology for resistance to the effects of single failures from exposure to heavy charged particles (TZZ) of outer space by irradiating a limited selection of LSIs with pulsed gamma-neutron ionizing radiation from a nuclear reactor or pulsed x-ray radiation from electrophysical installations (EFU) with equivalent dose, causing equal generation of radiation-induced charge in the sensitive volume of the LSI, equal to that of TZZ, characterized in that instead of independent irradiation, ha Ma-neutron radiation of the reactor, as well as protons, electrons and TZCh, irradiate only gamma-neutron radiation of a pulsed nuclear reactor (INR) with an average energy of 1.0-3.0 MeV or pulsed x-ray radiation of an electron diffraction device and to determine the resistance to TZCh with the value of the threshold value of linear energy losses LET in the range from units to hundreds of MeV · cm / g, the value of the coefficient of relative effectiveness RDEF (Relative Dose Enhancement Factor) of exposure to the full absorbed dose of x-ray or gamma radiation relative to the magnitude LETs using sootnosheniyav edinitsahgde ρ - density of the irradiated semiconductor material, g · cm, - the maximum chord in the chip MIS structure, cm; a is the chip width of the TIR structure, cm; b is the length of the chip, cm; c is the height of the chip; cm; is the constant of radiation generation of charge carriers, C · cmrad (M); is the limiting value of the fraction of unrecombined radiation-induced charge in the MIS structure when exposed to radiation from a simulator (MU) in the presence of an applied electric field of intensity E, MV · cm; - f �
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RU2578053C1 (en) * | 2014-09-22 | 2016-03-20 | Федеральное государственное унитарное предприятие федеральный научно-производственный центр "Научно-исследовательский институт измерительных систем им. Ю.Е. Седакова" | Method for evaluating resistance of digital electronic equipment to ionising radiation (versions) |
RU2657327C1 (en) * | 2016-12-26 | 2018-06-13 | Российская Федерация, от имени которой выступает Государственная корпорация по атомной энергии "Росатом" (Госкорпорация "Росатом") | Method for evaluating of the digital electronics elements stability to the effects of failures from the single particles influence |
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RU2082178C1 (en) * | 1995-03-21 | 1997-06-20 | Российский научно-исследовательский институт "Электронстандарт" | Method for selecting plates with radiation-resistant mos integrated circuits |
RU95111200A (en) * | 1995-06-28 | 1997-06-20 | Российский научно-исследовательский институт "Электронстандарт" | Method for testing bipolar semiconductor devices for resistance to ionizing space radiation |
RU2168735C2 (en) * | 1999-04-05 | 2001-06-10 | РНИИ "Электронстандарт" | Procedure of selection of electron articles by stability and reliability |
RU2169961C2 (en) * | 1999-09-27 | 2001-06-27 | Вовк Оксана Валерьевна | Semiconductor device test technique |
RU2178182C1 (en) * | 2000-07-03 | 2002-01-10 | Вовк Оксана Валерьевна | Process of testing of semiconductor devices |
US6914447B2 (en) * | 2003-04-23 | 2005-07-05 | Texas Instruments Incorporated | High activity, spatially distributed radiation source for accurately simulating semiconductor device radiation environments |
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RU2311654C2 (en) * | 2006-01-10 | 2007-11-27 | Государственное образовательное учреждение высшего профессионального образования Московский инженерно-физический институт (государственный университет) | Method for dividing integration microchips on basis of radiation resistance and reliability |
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Cited By (2)
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CN114414971A (en) * | 2021-12-14 | 2022-04-29 | 上海精密计量测试研究所 | Method for quantifying proton ionization damage based on dark current of CMOS image sensor |
CN114414971B (en) * | 2021-12-14 | 2024-05-28 | 上海精密计量测试研究所 | Method for quantifying proton ionization damage based on dark current of CMOS image sensor |
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