序号 | 专利名 | 申请号 | 申请日 | 公开(公告)号 | 公开(公告)日 | 发明人 |
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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. |
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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. |