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(火花室入H01J47/14);粒子轨迹的处理或分析〔2〕
序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
1 RADIATION DETECTION ELEMENT AND RADIATION DETECTION DEVICE US15994123 2018-05-31 US20180292546A1 2018-10-11 Tomohisa MOTOMURA; Kohei OTA; Toru TANIMORI; Atsushi TAKADA; Taito TAKEMURA
A radiation detection element includes a plurality of pixel electrodes, each pixel electrodes including a first electrode placed on the first surface of an insulating member and having an opening portion and a second electrode placed at the opening portion of the first electrode. The plurality of pixel electrodes is arrayed in the row direction and the column direction. The pitch of the pixel electrodes in the row direction and the column direction is 380 μm or less. An area ratio between the first electrode and the second electrode falls within the range of 14.5:1 to 154.6:1.
2 COMPOSITIONS AND METHODS FOR DETECTING RADIATION US15507509 2015-08-28 US20170248707A1 2017-08-31 Rusi P. Taleyarkhan
Tensioned metastable fluid detectors are disclosed that minimize false positive detection events. The methods involve the use of new fluids that provide improved neutron-alpha fission detection at reduced tension states. The rate of spin is also increased using a new protocol that avoids the creation of liquid imbalances in the arms of a CTMFD (centrifugally tensioned metastable fluid detector). The disclosed CTMFD radiation detection system includes a detector assembly containing a detection fluid, a base, a safety enclosure, a motor and motor mounting bracket, speed sensors, a cooling system that includes an air inlet and outlet and a safety enclosure. The CTMFD radiation detection system can include a plurality of independent detector arms having fluids with distinct Pneg requirements such that the range of detectable radiation is increased. Also disclosed are methods for detecting radiation using the disclosed CTMFD radiation detection system. Motor speed calibration procedures are also disclosed.
3 METHOD OF LUMINESCENT SOLID STATE DOSIMETRY OF MIXED RADIATIONS US12908051 2010-10-20 US20110031413A1 2011-02-10 Mark S. AKSELROD; Garrett J. Sykora
A method of determining the doses of neutrons, gamma and X-ray photons, beta, alpha and other ionizing radiations using a method of image processing in spatial and frequency domain that produces parameters that are related to the radiation dose absorbed in a luminescent material. Portions of the luminescent material may be covered by different converters to allow for doses of different radiations to be discriminated.
4 METHOD OF LUMINESCENT SOLID STATE DOSIMETRY OF MIXED RADIATIONS US12908043 2010-10-20 US20110031412A1 2011-02-10 Mark S. AKSELROD; Garrett J. Sykora
A method of determining the doses of neutrons, gamma and X-ray photons, beta, alpha and other ionizing radiations using a method of image processing in spatial and frequency domain that produces parameters that are related to the radiation dose absorbed in a luminescent material. Portions of the luminescent material may be covered by different converters to allow for doses of different radiations to be discriminated.
5 Process of making an imaging scintillation chamber US3507734D 1965-02-26 US3507734A 1970-04-21 RUDERMAN IRVING WARREN
6 METHOD AND APPARATUS FOR RADIATION DOSIMETRY UTILIZING FLUORESCENT IMAGING WITH PRECISION CORRECTION EP14811746 2014-02-11 EP3049826A4 2017-08-02 AKSELROD MARK S; BARTZ JAMES; DING FUJIAN; FOMENKO VASILIY V
A method comprising the following steps: (a) adjusting a radiation dose measurement for a fluorescent nuclear track detector based on a plurality of fluorescence contrast images for the fluorescent nuclear track detector to thereby produce a calibrated radiation dose measurement, and (b) displaying the calibrated radiation dose measurement to a user and/or saving the calibrated radiation dose measurement to a storage medium, wherein the fluorescent nuclear track detector comprises a luminescent material, wherein the radiation dose measurement is based on one or more fluorescent light measurements produced by fluorescent imaging of the fluorescent nuclear track detector using excitation light from a laser having a first wavelength, and wherein the plurality of fluorescence contrast images are produced by illuminating the fluorescent nuclear track detector with excitation light having a second wavelength.
7 METHOD OF LUMINESCENT SOLID STATE DOSIMETRY OF MIXED RADIATIONS EP09822675 2009-10-22 EP2340421A4 2014-05-21 AKSELROD MARK S; SYKORA GARRETT J
8 ミュオン軌跡検出器及びミュオン軌跡検出方法 JP2014004523 2014-01-14 JP6162610B2 2017-07-12 中山 幸一; 宮寺 晴夫; 吉岡 研一; 杉田 宰; 久米 直人; 伴 雄一郎
9 混合放射線のルミネセンス固体線量計測法 JP2011533315 2009-10-22 JP5643763B2 2014-12-17 エス. アクセルロッド,マーク; ジェイ. シーコラ,ガレット
10 Determination of the fissile material content in the small particle JP2000523568 1998-11-25 JP2001525550A 2001-12-11 ヘール ヤコブス ファン; アンドレ ラゲルワルト
(57)【要約】 本発明は、環境サンプルの如きサンプルに存在する小粒子中の核分裂性物質含量の定量法に係る。 本発明によれば、これ自体公知の「核分裂トラック」法を前記サンプルに適用し、サンプルを有機シート内にサンドイッチし、ついで、限定された熱中性子フルエンスに供する。 その際、サンプル中の核分裂性物質の核分裂生成物がシート内に核分裂トラックを創製する。 このトラックを化学エッチング法によって目視可能なものとする。 このようなトラックを創製した特定の粒子のサイズを好適な顕微鏡で測定し、その後、前記特定の粒子の目視可能なトラックを、異なる段階の既知のサイズ及び濃縮度の粒子から同じ方法によって得られた予め確立された標準トラックと比較する。
11 ELECTRONIC DEVICE SUBSTRATE AND METHOD FOR MANUFACTURING THE SAME US15436512 2017-02-17 US20170242137A1 2017-08-24 Claudia Sgiarovello; Martin Mischitz; Andrew Wood
A method for use in manufacturing a plurality of electronic devices from a workpiece. The method includes compiling a set of data records in a data file, wherein each data record represents information uniquely associated with a respective electronic device to be manufactured from the workpiece. Based on the data file, deposition of a substance is controlled at selected locations on the workpiece.
12 MUON TRACKER AND MUON TRACKING METHOD US14596637 2015-01-14 US20160377747A1 2016-12-29 Kohichi NAKAYAMA; Haruo MIYADERA; Kenichi YOSHIOKA; Tsukasa SUGITA; Naoto KUME; Yuichiro BAN
A muon tracker includes a drift tube detector having a plurality of drift tube arrays, a detection time-difference calculation circuit configured to calculate a detected time-difference between a plurality of time data detected at least two of the drift tubes, a time-difference information database that stores a relationship between a plurality of predetermined tracks of the muon passing the drift tube detector and a predetermined time-difference of possible detected time data to be detected at least two of the drift tubes where each of the plurality of predetermined tracks passes, a time-difference referring circuit configured to refer the detected time-difference calculated at the detection time-difference calculation circuit with the predetermined time-difference stored in the time-difference information database, and a muon track determining circuit configured to determine a muon track as the predetermined track of the muon corresponding to the predetermined time-difference that matches the best with the detected time-difference.
13 Method of luminescent solid state dosimetry of mixed radiations US12908043 2010-10-20 US07964854B2 2011-06-21 Mark S. Akselrod; Garrett J. Sykora
A method of determining the doses of neutrons, gamma and X-ray photons, beta, alpha and other ionizing radiations using a method of image processing in spatial and frequency domain that produces parameters that are related to the radiation dose absorbed in a luminescent material. Portions of the luminescent material may be covered by different converters to allow for doses of different radiations to be discriminated.
14 Method of luminescent solid state dosimetry of mixed radiations US12258035 2008-10-24 US07902525B2 2011-03-08 Mark S. Akselrod; Garrett J. Sykora
A method of determining the doses of neutrons, gamma and X-ray photons, beta, alpha and other ionizing radiations using a method of image processing in spatial and frequency domain that produces parameters that are related to the radiation dose absorbed in a luminescent material. Portions of the luminescent material may be covered by different converters to allow for doses of different radiations to be discriminated.
15 Detection of neutrons and heavy charged particles US10991456 2004-11-19 US07141804B1 2006-11-28 Mark Akselrod; R. Craig Yoder; Gleb Akselrod
The present invention provides a method and system for measuring the spatial distribution of fluorescence from the excited radiochromic luminescent material; and for signal processing of the spatial distribution of fluorescence to thereby detect tracks of one or more heavy charged particles with which the luminescent material has been irradiated. The present invention also provides a method and system for measuring the spatial distribution of fluorescence from an excited radiochromic luminescent material that has been irradiated with a hot particle of a radioactive material. The present invention provides a method for detecting thermal and fast neutrons as well as a method for determining parameters of heavy charge particles. In several embodiments of the present invention, the luminescent material comprises Al2O3 doped with magnesium and carbon.
16 Method for the quantitative determination of the fissile material content in small size particles US09555491 2000-06-01 US06459747B1 2002-10-01 Jacobus van Geel; André Lagerwaard
A method is provided for the quantitative determination of fissile material content in small size particles present in samples. 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 a microscope and thereafter these visible tracks of the selected particles are compared to pre-established standard tracks obtained by the same process from particles of different stepped known size and enrichment ratio.
17 Track registration detector for radon concentrations US703611 1991-05-21 US5132535A 1992-07-21 Daniel J. Steck
A detector for radon concentrations is provided having a housing, a cover member and a track registration device. The housing has a groove defined by a base, an inner wall and an outer wall with the inner wall and the outer wall extending from the base. The cover member has a side wall and is supported on the housing. The side wall intersects the groove thereby forming a U-shaped channel. The U-shaped channel creates a path for entry of radon concentrations from an exterior of the housing to an interior of the housing. The track registration mechanism is supported entirely within the housing and is capable of developing tracks thereon caused by radon-generated alpha particles.
18 Automated scanning of track recorders having variable track density US274850 1988-11-22 US4900935A 1990-02-13 James H. Roberts; Raymond Gold
A method is presented to scan fission tracks in solid state track recording material that provides a high degree of accuracy. Three separate methods of estimating true track density are used, each in its range of greatest reliability. The first method for low track density directly observes tracks and counts them. The second method for ranges of medial track density uses the Buffon needle method of determining the probability of track pile up to determine true track density. The third method, which is applicable at high track density, measures the amount of transmitted light to determine the opaque track area and relates this to true track density. The three methods are complimentary to each other and one of the set is automatically applied to any measured areal unit. The method is applied with known apparatus.
19 Solid-state track recorder dosimetry device to measure absolute reaction rates and neutron fluence as a function of time US72776 1987-07-13 US4874951A 1989-10-17 Raymond Gold; James H. Roberts
A solid state track recording type dosimeter is disclosed to measure the time dependence of the absolute fission rates of nuclides or neutron fluence over a period of time. In a primary species an inner recording drum is rotatably contained within an exterior housing drum that defines a series of collimating slit apertures overlying windows defined in the stationary drum through which radiation can enter. Film type solid state track recorders are positioned circumferentially about the surface of the internal recording drum to record such radiation or its secondary products during relative rotation of the two elements. In another species both the recording element and the aperture element assume the configuration of adjacent disks. Based on slit size of apertures and relative rotational velocity of the inner drum, radiation parameters within a test area may be measured as a function of time and spectra deduced therefrom.
20 Device for triggering a nuclear particle detector of the gas type US37232464 1964-06-03 US3373283A 1968-03-12 ALAIN LANSIART; JEAN LELOUP; JEAN LEQUAIS
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