首页 / 国际专利分类库 / 物理 / 测量 / 核辐射或X射线辐射的测量 / 粒子的运动或轨迹的记录 / .板或块,其中通过处理后核粒子的轨迹成为可见的,例如,利用照相乳胶,利用云母
序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
141 Radioactive decay products for the detector to be derived from the radon gas and radon gas JP2588088 1988-02-08 JP2567265B2 1996-12-25 ROBAATO UI FUIIRAA
142 JPH0528537Y2 - JP6196188 1988-05-10 JPH0528537Y2 1993-07-22
143 Manufacture of fissile deposit having selectively low mass for neutron dosimeter JP20359487 1987-08-18 JPS6350780A 1988-03-03 FURANSHISU HENRII RADEI
144 Method of measuring neutron dosage for prolonged term JP9425687 1987-04-16 JPS6348491A 1988-03-01 FURANSHISU HENRII RADEII
145 JPS6128952B2 - JP5494081 1981-04-11 JPS6128952B2 1986-07-03 HENRII WAADO ORUTA
146 Alpha-rays detector JP13441680 1980-09-29 JPS5760274A 1982-04-12 DOI HIROSHI
PURPOSE:To improve detecting sensitivity and detecting precision, by a method wherein a alpha-rays measuring device increases a pressure of a sample. CONSTITUTION:A large number of films 2 are housed in a measuring outer casing 5 enduring a pressure. Gas to be measured, pressurized by a pump, is fed through a feed valve 6 for measuring sample, e.g., gas. A pressure to be fed is measured by a pressure gauge 8. The films 2 are made of an organic compound resin, such as white mica, polycarbonate. When the gas is pressurized into a given pressure, the valve 6 closes. After it is left in said condition for a specific period, a valve 7 opens, and after the pressure goes to an atomospheric pressure, the films 2 are taken out. The films 2 are chemical-ground by means of a specific daustic soda at 70 deg.C for about 2hr, and this produces alpha-track on the films 2.
147 Method and device for reducing noises in investigation of uranium JP9908577 1977-08-18 JPS5323802A 1978-03-04 ROBAATO RUISU FUREISUCHIYAA
148 Device for reducing noises in investigation of uranium JP9908477 1977-08-18 JPS5323801A 1978-03-04 UIRIAMU JIESATSUPU WAADO ZA SA
149 JPS5032719B1 - JP9399069 1969-11-25 JPS5032719B1 1975-10-23
150 JPS5017277B1 - JP9651370 1970-11-04 JPS5017277B1 1975-06-19
151 JPS4986080A - JP7923173 1973-07-13 JPS4986080A 1974-08-17
152 JPS4927071B1 - JP4503768 1968-06-29 JPS4927071B1 1974-07-15
153 JPS4964483A - JP6647073 1973-06-14 JPS4964483A 1974-06-21
154 JPS4836915B1 - JP10209370 1970-11-20 JPS4836915B1 1973-11-07
155 NOVEL RADIATION DETECTOR EP11791625.4 2011-11-28 EP2643708B1 2015-01-14 STANLEY, Steven John; HORSFALL, John Paul Owen
156 NOVEL RADIATION DETECTOR EP11791625.4 2011-11-28 EP2643708A2 2013-10-02 STANLEY, Steven John; HORSFALL, John Paul Owen
The invention provides a device for the detection and mapping of radiation, the device comprising a polymeric core located within an external shell material, wherein the polymeric core comprises a plurality of stacked polymeric sheets comprising at least one radiation sensitive component which is sensitive to said radiation emitted by said radioactive materials and the external sheath comprises a collimation sheath. Preferably, the polymeric core comprises a cubic, cylindrical, spherical or truncated spherical shape which is encased within the external shell. The external shell is preferably comprised of a metal, most preferably tungsten. The invention also provides a method for the detection and mapping of radiation in a location, which comprises: (a) placing a device according to the invention in the location to be investigated; (b) allowing the device to remain in the location and be exposed to the radiation for a predetermined length of time; (c) removing the device from the location; (d) removing the polymeric core from the external shell; (e) analysing said polymeric core by means of an optical analysis technique applying a software-based image reconstruction algorithm to image the polymeric core; and (f) determining the location, form and intensity of said radiation by further software-based analysis. The device and method of the invention facilitate the detection and mapping of radiation, and find particular use in mapping the location, intensity and identity of radiological hazards in 3 dimensions in sites such as active cells, gloveboxes, other active plants and confined spaces. Advantages over the prior art include significantly improved radiation sensitivity, the lack of requirement for an electrical supply, and the ability to deal with high radiation backgrounds and to be deployed in confined or restricted spaces.
157 A METHOD OF AUTOMATICALLY COUNTING FISSION TRACKS EP07784679.8 2007-07-25 EP2044463A1 2009-04-08 GLEADOW, Andrew, John, Ward
The present invention relates generally to the task of automatically counting the fission track density in a prepared crystal. Two images are captured by a charged coupled device (CCD) (16) attached to a microscope (14). The first or reflected light image (18) is of the surface of the crystal (12), the light captured by the CCD (16) having been reflected from the crystal surface. The reflected light image (18) is a RGB image of a prepared crystal of mica (12) containing surface voids corresponding to etched fission tracks. The second or transmitted light image (24) is of a plane near the surface of the crystal (12). The transmitted lighting image (24) is generally the same view as the reflected light image (18). A fission track void can be detected by comparing the reflected light (18) and the transmitted light (24) images. This comparison of the reflected light and the transmitted light images is best achieved using a computer software program, although this can also be done by a person comparing the images side by side or visually superimposing one on top of the other.
158 A method for determining quantitatively the content of fissile material in small size particles EP97121136.2 1997-12-02 EP0921415A1 1999-06-09 van Geel, Jacobus,Prof.Dr.; Lagerwaard, André

This invention refers to a method for the quantitative determination of the fissile material content in small size particles present in samples such as environmental samples. According to the invention, the "fission track process", known per se, is applied to said samples, according to which the samples are sandwiched in organic sheets and then submitted to a defined thermal neutron fluence whereupon fission products of the fissile material in the sample create in the sheets fission tracks which are rendered visible by etching the sheets.

Then the size of selected particles having created such tracks is determined by means of an appropriate microscope and thereafter these visible tracks of said selected particles are compared to pre-established standard tracks obtained by the same process from particles of different stepped known size and enrichment ratio.

159 Détecteur passif de rayonnement EP89110066.1 1989-06-03 EP0349771B1 1993-08-18 Andru, Jean, Antoine, Alphonse
160 Method for detecting and quantifying impurity actinides on fissionable deposits EP87307306.8 1987-08-18 EP0256884A3 1992-03-04 Gold, Raymond; Roberts, James Herbert; Ruddy, Francis Henry

A method is described for determining the amount and spatial distribution of impurity actinides in fission­able deposits used for measurement of solid state track recorder fission rate and neutron fluence. For example, a ²³⁹Pu fissionable deposit is autoradiographed with an alpha particle-sensitive track recorder which is then subjected to a four hour etch at room temperature. The etch induc­tion time for the ²³⁹Pu alpha particles is just barely exceeded, so that the²³⁹Pu tracks appear as very immature dots on the surface of the solid state track recorder. The ²³⁵U tracks, on the other hand, are correspondingly etched longer than their respective shorter etch induction time and appear as much more mature, longer tracks. The amounts of ²³⁵U and ²³⁹Pu present can be calculated from the numbers of different tracks that are counted.

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