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WO2018139954A1 - Sealed isotopic source of fission fragments based on californium-252 and a method of producing same - Google Patents

Sealed isotopic source of fission fragments based on californium-252 and a method of producing same Download PDF

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WO2018139954A1
WO2018139954A1 PCT/RU2017/000930 RU2017000930W WO2018139954A1 WO 2018139954 A1 WO2018139954 A1 WO 2018139954A1 RU 2017000930 W RU2017000930 W RU 2017000930W WO 2018139954 A1 WO2018139954 A1 WO 2018139954A1
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california
source
substrate
fission
sealed
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Андрей Николаевич СМИРНОВ
Владимир Владимирович ОБНОРСКИЙ
Татьяна Евгеньевна КУЗЬМИНА
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Akcionernoe Obshhestvo "radievyy Institut Imeni VG Khlopina"
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Akcionernoe Obshhestvo "radievyy Institut Imeni VG Khlopina"
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    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21GCONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
    • G21G4/00Radioactive sources
    • G21G4/04Radioactive sources other than neutron sources

Definitions

  • the invention relates to the field of physical chemistry of the surface and can be used in the manufacture of sources of fission fragments of a large area used in applied nuclear physics.
  • the invention in order to calibrate and determine the effectiveness of threshold fission fragment detectors in the study of stimulated fission of nuclei by neutrons, protons, gamma rays, etc. in a wide energy range, it is necessary to use spontaneous fission fragment sources with a uniform distribution of the active layer over an area of several cm 2 and an energy spectrum, with the separation of fragments into heavy and light groups.
  • sources of radioactive radiation must be sealed and ensure their mechanical strength. It should be noted that fission fragments during braking in a substance lose a unit of length more energy than other types of radioactive radiation (alpha, beta, gamma) and, accordingly, more intensively destroy protective coatings. With a relatively small surface activity of the source ( ⁇ 100 divisions per cm), a thin film of alumina (100 ⁇ g / cm thick) can serve as a protective coating, which does not pass heavy recoil nuclei and at the same time allows the spectrometric properties of the source to be preserved.
  • California the spontaneously fissile isotope Cf-252, hereinafter referred to as "California", is used.
  • the disadvantage of this method is that in the absence of sealing, the resulting active layer has weak adhesion to the surface of the substrate, can be easily mechanically removed from the substrate, and can also fade with time under the influence of its own self-dispersion.
  • Closest to the proposed invention are a device and a method of manufacturing a sealed source of fission fragments, in which a layer of gold ⁇ 1 ⁇ g / cm thick with a diameter equal to the diameter of the active spot ⁇ 3 mm is deposited on the substrate, onto which radiochemically pure California is deposited as a drop and after after drying the droplet, a sealing layer of nickel 1 mg / cm 2 thick is applied (. Patent Ru 2207639 (06/27/2003). Bull. 8).
  • the disadvantages of this device and method are the limited geometric size of the active spot of California-252, mechanically weak coating with a nickel film, and the relatively low quality of the spectrum of fission fragments, the energy loss of which is about 30 MeV.
  • the proposed inventions solve the problem of manufacturing a sealed source of fission fragments having a large active layer area and an energy spectrum of fragments with separation into heavy and light groups, with a minimum consumption of fissile material.
  • the proposed device includes an aluminum substrate, a layer of California-252 deposited on the entire surface of the substrate and a sealing film of aluminum oxide formed on top of it.
  • a method of manufacturing such a source is that a California-252 layer is deposited by desorption of a substance under the action of its own fission fragments (self-spraying) in vacuum from the mother source by scanning on the entire surface of the aluminum substrate, after which a sealing layer of aluminum oxide is formed (A1 2 0 3 ) by applying an aluminum layer over a layer of California, calcining the substrate with the deposited layers at a temperature close to the melting temperature of aluminum and subsequent anodic oxidation.
  • Figure 1 of the drawing shows a diagram of the proposed source device.
  • the source includes an aluminum substrate 1, an active layer of California, occupying almost the entire area of the substrate 2 and a sealing layer of aluminum oxide 3.
  • the proposed method of manufacturing a source of fission fragments is carried out in the following sequence.
  • an aluminum foil substrate is prepared, the surface of which is passivated by boiling in concentrated nitric acid.
  • California-252 is deposited onto the surface of the substrate by self-spraying with maternal source in a vacuum.
  • the deposition is carried out within the required area of the active spot by gradually moving the substrate (scan) in order to obtain a uniformly distributed layer and for a time determined by the deposition rate and the required value of the obtained activity.
  • After deposition of the California-252 layer, its total activity, the spectrum of fragments, and the uniformity of the activity distribution are measured using a semiconductor spectrometer.
  • the substrate with a layer of California-252 deposited on it is coated with a ⁇ 100 ⁇ g / cm thick aluminum layer by vacuum deposition.
  • the entire composition — the substrate with the deposited layers of California-252 and aluminum — is heated in vacuum to a temperature close to the melting temperature of aluminum ( ⁇ 650 ° C) in order to obtain good adhesion of the said layers to the substrate.
  • an oxide film is carried out by the method of anodic oxidation.
  • the substrate is immersed in an electrolytic cell with an ammonium solution, to the electrodes of which a voltage of about 200 volts is applied.
  • the substrate is washed in distilled water and dried.
  • the total activity, the spectrum of alpha particles and fission fragments, and the uniformity of the activity distribution are measured using a semiconductor spectrometer.
  • the verification is periodically repeated.
  • a 10 6 6 Torr self-spraying method in a 10 6 6 Torr vacuum foil from a parent source weighing ⁇ 0.5 ⁇ g was applied to a substrate of aluminum foil 0.1 mm thick, treated in boiling nitric acid, by applying a 15x15 mm California layer by moving the substrate relative to the parent source.
  • the substrate was placed in an electrolytic cell, the voltage of -200 V was applied to the electrodes of the cell.
  • the electrolysis process was controlled by measuring the current.
  • the substrate was washed in distilled water and dried.
  • FIG. Figure 2 shows the energy spectra of fission fragments emitted from the active layer deposited in the process of self-atomization of the mother source, before (curve 1) and after the formation of a sealing film of aluminum oxide and drying of the substrate (curve 2).
  • the shift of the spectrum after the formation of the oxide film relative to the reference one is on average about 7 MeV, which corresponds to the inhibitory energy loss of fragments in the alumina layer with a thickness of about 0.4 ⁇ m.
  • FIG. Figure 3 shows source samples made by the above method.
  • the source leak test was carried out once every 3 months for one year. In each cycle, a clean aluminum collector was placed above the source through a 0.5 mm thick spacer ring. The assembly was heated under vacuum of 10 "6 torr for 2 days, then collection was measured on the alpha-spectrometer. Pulses corresponding alpha activity on the surface of collections in the alpha-peak californium-252, at this stage test were observed, which testified to the tightness of the source.

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  • Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • General Chemical & Material Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Measurement Of Radiation (AREA)
  • Other Surface Treatments For Metallic Materials (AREA)

Abstract

The inventions relate to the field of surface science and may be used in the production of sources of fission fragments with a large area that can be used in applied nuclear physics, e.g. to calibrate and determine the effectiveness of threshold detectors of fission fragments when studying the induced fission of nuclei by neutrons, protons, gamma quanta, etc. in a broad range of energies. A device and a method of producing a sealed isotopic source of fission fragments based on californium-252 consists in depositing californium-252 on an aluminium substrate by desorbing the substance by exposure to its own fission fragments (self-sputtering), and then forming a sealing layer of aluminium oxide (Al2O3). The proposed inventions solve the problem of producing a sealed and stable fissile-fragment source that has an energy spectrum of fragments that are separated into heavy and light groups, with minimal consumption of the fissile substance.

Description

ГЕРМЕТИЧНЫЙ ИЗОТОПНЫЙ ИСТОЧНИК ОСКОЛКОВ ДЕЛЕНИЯ НА ОСНОВЕ КАЛИФОРНИЯ-252 И СПОСОБ ЕГО ИЗГОТОВЛЕНИЯ  SEALED ISOTOPIC SOURCE OF FISSION SHARES BASED ON CALIFORNIA-252 AND METHOD FOR ITS MANUFACTURE

Изобретения относятся к области физикохимии поверхности и могут быть использованы при изготовлении источников осколков деления большой площади, применяемых в прикладной ядерной физике. Например, для калибровки и определения эффективности пороговых детекторов осколков деления при исследовании вынужденного деления ядер нейтронами, протонами, гамма-квантами и др. в широкой области энергий необходимо использовать источники осколков спонтанного деления с равномерным распределением активного слоя на площади несколько см2 и энергетическим спектром, с разделением осколков на тяжелую и легкую группы. The invention relates to the field of physical chemistry of the surface and can be used in the manufacture of sources of fission fragments of a large area used in applied nuclear physics. For example, in order to calibrate and determine the effectiveness of threshold fission fragment detectors in the study of stimulated fission of nuclei by neutrons, protons, gamma rays, etc. in a wide energy range, it is necessary to use spontaneous fission fragment sources with a uniform distribution of the active layer over an area of several cm 2 and an energy spectrum, with the separation of fragments into heavy and light groups.

Для предотвращения утечки активного вещества и загрязнения окружающей среды источники радиоактивных излучений необходимо герметизировать и обеспечивать их механическую прочность. Следует отметить, что осколки деления при торможении в веществе теряют на единицу длины больше энергии, чем другие виды радиоактивных излучений (альфа-, бета-, гамма-) и, соответственно, более интенсивно разрушают защитные покрытия. При сравнительно небольшой поверхностной активности источника (~ 100 делений на см ) в качестве защитного покрытия может служить тонкая пленка окиси алюминия (толщиной - 100 мкг/см ), которая не пропускает тяжелые ядра отдачи и в то же время позволяет сохранить спектрометрические свойства источника.  To prevent leakage of the active substance and environmental pollution, sources of radioactive radiation must be sealed and ensure their mechanical strength. It should be noted that fission fragments during braking in a substance lose a unit of length more energy than other types of radioactive radiation (alpha, beta, gamma) and, accordingly, more intensively destroy protective coatings. With a relatively small surface activity of the source (~ 100 divisions per cm), a thin film of alumina (100 μg / cm thick) can serve as a protective coating, which does not pass heavy recoil nuclei and at the same time allows the spectrometric properties of the source to be preserved.

В рассматриваемых источниках осколков деления используют спонтанно делящийся изотоп Cf-252, именуемый ниже "калифорний".  In the sources of fission fragments under consideration, the spontaneously fissile isotope Cf-252, hereinafter referred to as "California", is used.

Известен способ изготовления источников осколков деления, в котором осаждение калифорния производят методом самораспыления материнского слоя на металлическую подложку (R. С. Gatti, L. Phillips, IIR. Bowman and S. G. Thompson. "Self-transfer of Cf- 252". UCRL-9093 (1960); S. Pauker and N. H. Steiger-Shafrir. Transfer properties of 252Cf and their use for source preparation. . Nucl. Instr. & Meth. 91 (1971) 557-563). A known method of manufacturing sources of fission fragments, in which the deposition of California is carried out by self-spraying the mother layer on a metal substrate (R. C. Gatti, L. Phillips, IIR. Bowman and SG Thompson. "Self-transfer of Cf-252." UCRL-9093 (1960); S. Pauker and NH Steiger-Shafrir. Transfer properties of 252 Cf and their use for source preparation. Nucl. Instr. & Meth. 91 (1971) 557-563).

Недостатком этого способа является то, что в отсутствие герметизации полученный активный слой имеет слабое сцепление с поверхностью подложки, может быть легко механически удален с подложки, а также может улетучиваться со временем под действием собственного самораспыления. Наиболее близким к предлагаемому изобретению являются устройство и способ изготовления герметичного источника осколков деления, в котором на подложку наносят слой золота толщиной ~ 1 мкг/см с диаметром, равным диаметру активного пятна ~ 3 мм , на который осаждают в виде капли радиохимически чистый калифорний и после высыхания капли наносят герметизирующий слой из никеля толщиной 1 мг/см2 (. Патент Ru 2207639 (27.06.2003). Бюл. 8). The disadvantage of this method is that in the absence of sealing, the resulting active layer has weak adhesion to the surface of the substrate, can be easily mechanically removed from the substrate, and can also fade with time under the influence of its own self-dispersion. Closest to the proposed invention are a device and a method of manufacturing a sealed source of fission fragments, in which a layer of gold ~ 1 μg / cm thick with a diameter equal to the diameter of the active spot ~ 3 mm is deposited on the substrate, onto which radiochemically pure California is deposited as a drop and after after drying the droplet, a sealing layer of nickel 1 mg / cm 2 thick is applied (. Patent Ru 2207639 (06/27/2003). Bull. 8).

Недостатками этого устройства и способа являются ограниченный геометрический размер активного пятна калифорния-252, механически непрочное покрытие никелевой пленкой, а также сравнительно невысокое качество спектра осколков деления, потери энергий которых составляют около 30 МэВ.  The disadvantages of this device and method are the limited geometric size of the active spot of California-252, mechanically weak coating with a nickel film, and the relatively low quality of the spectrum of fission fragments, the energy loss of which is about 30 MeV.

Предлагаемыми изобретениями решается задача изготовления герметичного источника осколков деления, имеющего большую площадь активного слоя и энергетический спектр осколков с разделением на тяжелую и легкую группы, при минимальном расходе делящегося вещества.  The proposed inventions solve the problem of manufacturing a sealed source of fission fragments having a large active layer area and an energy spectrum of fragments with separation into heavy and light groups, with a minimum consumption of fissile material.

Предлагаемое устройство включает алюминиевую подложку, нанесенный на всю поверхность подложки слой калифорния-252 и сформированную поверх него герметизирующую пленку из оксида алюминия.  The proposed device includes an aluminum substrate, a layer of California-252 deposited on the entire surface of the substrate and a sealing film of aluminum oxide formed on top of it.

Способ изготовления такого источника заключается в том, что слой калифорния-252 осаждают методом десорбции вещества под действием собственных осколков деления (самораспыления) в вакууме с материнского источника путем сканирования на всю поверхность алюминиевой подложки, после чего формируют герметизирующий слой из окисла алюминия (А1203) путем нанесения слоя алюминия поверх слоя калифорния, прокаливания подложки с нанесенными слоями при температуре близкой к температуре плавления алюминия и последующим анодным оксидированием. A method of manufacturing such a source is that a California-252 layer is deposited by desorption of a substance under the action of its own fission fragments (self-spraying) in vacuum from the mother source by scanning on the entire surface of the aluminum substrate, after which a sealing layer of aluminum oxide is formed (A1 2 0 3 ) by applying an aluminum layer over a layer of California, calcining the substrate with the deposited layers at a temperature close to the melting temperature of aluminum and subsequent anodic oxidation.

На фиг.1 чертежа представлена схема предлагаемого устройства источника. Источник включает в себя алюминиевую подложку 1, активный слой калифорния, занимающий почти всю площадь подложки 2 и герметизирующий слой из окиси алюминия 3. Figure 1 of the drawing shows a diagram of the proposed source device. The source includes an aluminum substrate 1, an active layer of California, occupying almost the entire area of the substrate 2 and a sealing layer of aluminum oxide 3.

Предлагаемый способ изготовления источника осколков деления осуществляют в следующей последовательности.  The proposed method of manufacturing a source of fission fragments is carried out in the following sequence.

Вначале производится подготовка подложки из алюминиевой фольги, поверхность которой пассивируют путем кипячения в концентрированной азотной кислоте. Затем на поверхность подложки осаждают калифорний-252 методом самораспыления с материнского источника в вакууме. Осаждение проводят в пределах требуемой площади активного пятна путем постепенного перемещения подложки (сканирования) с целью получения равномерно распределенного слоя и в течение времени, определяемого скоростью осаждения и требуемой величиной полученной активности. После осаждения слоя калифорния-252 измеряют его общую активность, спектр осколков и равномерность распределения активности с помощью полупроводникового спектрометра. First, an aluminum foil substrate is prepared, the surface of which is passivated by boiling in concentrated nitric acid. Then, California-252 is deposited onto the surface of the substrate by self-spraying with maternal source in a vacuum. The deposition is carried out within the required area of the active spot by gradually moving the substrate (scan) in order to obtain a uniformly distributed layer and for a time determined by the deposition rate and the required value of the obtained activity. After deposition of the California-252 layer, its total activity, the spectrum of fragments, and the uniformity of the activity distribution are measured using a semiconductor spectrometer.

Далее подложку с нанесенным на нее слоем калифорния-252 покрывают слоем алюминия толщиной ~ 100 мкг/см путем напыления в вакууме. После этого всю композицию - подложку с нанесенными слоями калифорния-252 и алюминия прогревают в вакууме до температуры, близкой к температуре плавления алюминия (~650°С) с целью получения хорошего сцепления упомянутых слоев с подложкой.  Next, the substrate with a layer of California-252 deposited on it is coated with a ~ 100 μg / cm thick aluminum layer by vacuum deposition. After that, the entire composition — the substrate with the deposited layers of California-252 and aluminum — is heated in vacuum to a temperature close to the melting temperature of aluminum (~ 650 ° C) in order to obtain good adhesion of the said layers to the substrate.

Формирование пленки окисла осуществляют методом анодного оксидирования. Для этого подложку погружают в электролитическую ячейку с раствором аммония, к электродам которой прикладывают напряжение около 200 Вольт. По окончании электролиза подложку промывают в дистиллированной воде и сушат. После формирования окисной пленки измеряют общую активность, спектр альфа-частиц и осколков деления и равномерность распределения активности с помощью полупроводникового спектрометра.  The formation of an oxide film is carried out by the method of anodic oxidation. For this, the substrate is immersed in an electrolytic cell with an ammonium solution, to the electrodes of which a voltage of about 200 volts is applied. At the end of electrolysis, the substrate is washed in distilled water and dried. After the formation of the oxide film, the total activity, the spectrum of alpha particles and fission fragments, and the uniformity of the activity distribution are measured using a semiconductor spectrometer.

Проверку изготовленного источника на герметичность производят следующим образом. На расстоянии 0,2-0,3 мм от поверхности источника располагают чистую алюминиевую фольгу и сборку "источник - фольга" помещают в вакуум. После определенной экспозиции измеряют альфа-активность на поверхности фольги в области альфа-пика калифорния.  Check the manufactured source for leaks as follows. At a distance of 0.2-0.3 mm from the surface of the source, a clean aluminum foil is placed and the source-foil assembly is placed in a vacuum. After a certain exposure, alpha activity is measured on the surface of the foil in the alpha peak region of California.

Проверку изготовленного источника на механическую прочность поверхности производят путем «мазков» ватными тампонами и последующих измерений альфа- активности тампона.  The manufactured source is checked for the mechanical strength of the surface by “swabs” with cotton swabs and subsequent measurements of the alpha activity of the swab.

В процессе эксплуатации источника проверку периодически повторяют.  During operation of the source, the verification is periodically repeated.

Пример. Example.

На подложку из алюминиевой фольги толщиной 0.1 мм, обработанной в кипящей азотной кислоте, методом самораспыления в вакууме 10"6 Торр с материнского источника весом ~ 0.5 мкг наносили слой калифорния площадью 15x15 мм путем перемещения подложки относительно материнского источника. A 10 6 6 Torr self-spraying method in a 10 6 6 Torr vacuum foil from a parent source weighing ~ 0.5 μg was applied to a substrate of aluminum foil 0.1 mm thick, treated in boiling nitric acid, by applying a 15x15 mm California layer by moving the substrate relative to the parent source.

з Поверх слоя калифорния методом термического испарения в вакууме осаждали слой алюминия толщиной ~100 мкг/см и затем, не нарушая вакуума, подложку со слоями калифорния и напыленного алюминия прогревали до температуры, близкой к температуре плавления алюминия (~ 650°С). s A ~ 100 μg / cm thick aluminum layer was deposited by vacuum thermal evaporation on top of a California layer, and then, without violating the vacuum, the substrate with layers of California and deposited aluminum was heated to a temperature close to the melting temperature of aluminum (~ 650 ° C).

После этого подложку помещали в электролитическую ячейку, к электродам которой прикладывали напряжение -200 В. Процесс электролиза контролировали измерением тока. По окончании электролиза подложку промывали в дистиллированной воде и высушивали.  After that, the substrate was placed in an electrolytic cell, the voltage of -200 V was applied to the electrodes of the cell. The electrolysis process was controlled by measuring the current. At the end of electrolysis, the substrate was washed in distilled water and dried.

На фиг. 2 чертежа представлены энергетические спектры осколков деления, вылетающих из активного слоя, нанесенного в процессе самораспыления материнского источника, до (кривая 1) и после формирования герметизирующей пленки окисла алюминия и высыхания подложки (кривая 2).  In FIG. Figure 2 shows the energy spectra of fission fragments emitted from the active layer deposited in the process of self-atomization of the mother source, before (curve 1) and after the formation of a sealing film of aluminum oxide and drying of the substrate (curve 2).

Энергетический спектр осколков деления, вылетающих из активного пятна без покрытия практически не отличается от эталонного (P. Wolilfarth et al. Pulse height defect of fission fragment products in a silicon surface barrier detector. . Nucl. Instr. & Meth. 140 (1977) 189-191).  The energy spectrum of fission fragments emitted from an active spot without a coating is practically the same as the reference one (P. Wolilfarth et al. Pulse height defect of fission fragment products in a silicon surface barrier detector. Nucl. Instr. & Meth. 140 (1977) 189 -191).

Сдвиг спектра после формирования оксидной пленки относительно эталонного составляет в среднем около 7 МэВ, что соответствует тормозным потерям энергии осколков в слое окиси алюминия толщиной около 0.4 мкм.  The shift of the spectrum after the formation of the oxide film relative to the reference one is on average about 7 MeV, which corresponds to the inhibitory energy loss of fragments in the alumina layer with a thickness of about 0.4 μm.

На фиг. 3 чертежа показаны образцы источников, изготовленные вышеописанным способом  In FIG. Figure 3 shows source samples made by the above method.

Проверку герметичности источника проводили один раз в 3 месяца в течение одного года. В каждом цикле чистый алюминиевый сборник располагали над источником через разделительное кольцо толщиной 0,5 мм. Сборку выдерживали в вакууме 10"6 Торр в течение 2-х суток, а затем сборник измеряли на альфа-спектрометре. Импульсов, соответствующих альфа-активности на поверхности сборников в области альфа-пика калифорния-252, на этой стадии проверки отмечено не было, что свидетельствовало о герметичности источника. The source leak test was carried out once every 3 months for one year. In each cycle, a clean aluminum collector was placed above the source through a 0.5 mm thick spacer ring. The assembly was heated under vacuum of 10 "6 torr for 2 days, then collection was measured on the alpha-spectrometer. Pulses corresponding alpha activity on the surface of collections in the alpha-peak californium-252, at this stage test were observed, which testified to the tightness of the source.

Периодические измерения активности источника на протяжении одного года показали уменьшение активности в точном соответствии с периодом полураспада калифорния-252 (2.64 года).  Periodic measurements of the activity of the source over one year showed a decrease in activity in exact accordance with the half-life of California-252 (2.64 years).

Claims

Формула изобретения Claim 1. Герметичный изотопный источник осколков деления на основе калифорния-252, включающий подложку с нанесенным на нее активным слоем и герметизирующим слоем, отличающийся тем, что активный слой калифорния-252, распределен на всю поверхность алюминиевой подложки, а герметизирующим слоем является окись алюминия.  1. A sealed isotope source of fission fragments based on California-252, including a substrate with an active layer deposited on it and a sealing layer, characterized in that the active layer of California-252 is distributed over the entire surface of the aluminum substrate, and the sealing layer is aluminum oxide. 2. Способ изготовления герметичного изотопного источника осколков деления на основе калифорния-252, включающий осаждение калифорния-252 на подложку и формирование герметизирующего слоя, отличающийся тем, что осаждение калифорния- 252 проводят методом самораспыления в вакууме с материнского источника путем сканирования на всю поверхность алюминиевой подложки, а формирование герметизирующего слоя из окиси алюминия осуществляют путем нанесения слоя алюминия поверх слоя калифорния-252, прокаливания алюминиевой подложки с нанесенными слоями при температуре близкой к температуре плавления алюминия и последующим анодным оксидированием.  2. A method of manufacturing a sealed isotope source of fission fragments based on California-252, including the deposition of California-252 on the substrate and the formation of the sealing layer, characterized in that the deposition of California-252 is carried out by self-spraying in vacuum from the mother source by scanning on the entire surface of the aluminum substrate and the formation of a sealing layer of aluminum oxide is carried out by applying an aluminum layer over a layer of California-252, calcining an aluminum substrate with deposited layers When a temperature near the melting temperature of aluminum and subsequent anodic oxidation.
PCT/RU2017/000930 2017-01-27 2017-12-12 Sealed isotopic source of fission fragments based on californium-252 and a method of producing same Ceased WO2018139954A1 (en)

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RU2207639C2 (en) * 2001-05-03 2003-06-27 Государственное унитарное предприятие Научно-производственное объединение "Радиевый институт им. В.Г.Хлопина" Sealed isotope source of californium base fission fragments and its manufacturing process
US20130302236A1 (en) * 2009-09-28 2013-11-14 John J. Munro, III Gamma radiation source
RU2558660C1 (en) * 2014-03-14 2015-08-10 Открытое акционерное общество "Радиевый институт имени В.Г. Хлопина" Sealed isotope source of fission fragments based on californium-252 and method of producing same

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RU2207639C2 (en) * 2001-05-03 2003-06-27 Государственное унитарное предприятие Научно-производственное объединение "Радиевый институт им. В.Г.Хлопина" Sealed isotope source of californium base fission fragments and its manufacturing process
US20130302236A1 (en) * 2009-09-28 2013-11-14 John J. Munro, III Gamma radiation source
RU2558660C1 (en) * 2014-03-14 2015-08-10 Открытое акционерное общество "Радиевый институт имени В.Г. Хлопина" Sealed isotope source of fission fragments based on californium-252 and method of producing same

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