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    • 1. 发明专利
    • Radon concentration measuring device
    • RADON浓度测量装置
    • JP2010008140A
    • 2010-01-14
    • JP2008165675
    • 2008-06-25
    • Chubu Electric Power Co IncOhyo Koken Kogyo Co Ltd中部電力株式会社応用光研工業株式会社
    • NISHIMOTO AKIYOSHISHIMO MICHIKUNIKONISHI TOSHIHARU
    • G01T1/167G01T1/16
    • PROBLEM TO BE SOLVED: To provide a radon concentration measuring device dispensing with use of not only a pump or a fan but also a power source for driving the pump or the fan, capable of replacing easily the air which is a measuring object for radon concentration. SOLUTION: This radon concentration measuring device 100 includes a radon concentration measuring device body 110, an air taking apparatus 120 for taking the air which is the measuring object for radon concentration, and a support tool 130 arranged below the radon concentration measuring device body 110 and having a bottom surface 132 for supporting the air taking apparatus 120. The air taking apparatus 120 has an extraction structure which is slidable so as to be openable/closable relative to the radon concentration measuring device body 110 and the support tool 130. The air taking apparatus 120 has a peripheral wall 121 forming a closed cross section, and is opened vertically. COPYRIGHT: (C)2010,JPO&INPIT
    • 要解决的问题:为了提供不仅使用泵或风扇而且使用用于驱动泵或风扇的电源的氡浓度测量装置,其能够容易地更换作为测量对象的空气 用于氡浓度。 解决方案:该氡浓度测量装置100包括氡浓度测量装置主体110,用于吸收作为氡浓度的测量对象的空气的取气装置120和布置在氡浓度测量装置下方的支撑工具130 主体110并且具有用于支撑取气装置120的底表面132.取气装置120具有可相对于氡浓度测量装置主体110和支撑工具130可开启和关闭的抽出结构。 取气装置120具有形成封闭截面的周壁121,并且垂直地打开。 版权所有(C)2010,JPO&INPIT
    • 2. 发明专利
    • Scintillation detector
    • SCINTILLATION检测器
    • JP2008039548A
    • 2008-02-21
    • JP2006213206
    • 2006-08-04
    • Ohyo Koken Kogyo Co Ltd応用光研工業株式会社
    • YAMAMOTO TATSUOTAKASO TATSUMIFUKUZAWA AKIRA
    • G01T1/208C09K11/00C09K11/80G01T1/20
    • PROBLEM TO BE SOLVED: To provide a scintillation detector that will not have average DC level from varying, even with respect to significant changes in the luminance of incident radiation.
      SOLUTION: A negative bias voltage is applied to a photocathode K from a bias power supply terminal 6, in order to bring the anode A of a photomultiplier tube 2 to be at the zero potential. Rather than DC coupling, AC coupling using a capacitor is configured in each of signal paths between the output of the photomultiplier tube 2 and the input of a DC-type waveform shaping amplifier 3, and between an output of the DC-type waveform shaping amplifier 3 and an output terminal 5 of the scintillation detector.
      COPYRIGHT: (C)2008,JPO&INPIT
    • 要解决的问题:即使对于入射辐射的亮度的显着变化,也提供不具有平均DC电平变化的闪烁检测器。 解决方案:为了使光电倍增管2的阳极A处于零电位,从偏压电源端子6向负电偏压施加负偏压。 而不是DC耦合,使用电容器的AC耦合被配置在光电倍增管2的输出和DC型波形整形放大器3的输入之间的每个信号路径中,并且在DC型波形整形放大器 3和闪烁检测器的输出端子5。 版权所有(C)2008,JPO&INPIT
    • 5. 发明专利
    • Method and device for measuring radiation dose
    • 用于测量辐射剂量的方法和装置
    • JP2010169645A
    • 2010-08-05
    • JP2009014790
    • 2009-01-26
    • Natl Inst Of Radiological SciencesOhyo Koken Kogyo Co Ltd応用光研工業株式会社独立行政法人放射線医学総合研究所
    • WATAI KATSUNORIKAMATA TAKASHISHIRAKAWA YOSHIYUKI
    • G01T1/169
    • PROBLEM TO BE SOLVED: To provide a radiation dose measuring method for predicting, calculating and displaying the final response value of a radiation dose measuring device, without having to wait for the lapse of time constant, and to provide a prediction-corresponding type radiation dose measuring device. SOLUTION: This radiation dose measuring device includes an output section for generating an output pulse due to incidence of radiation; a counting rate arithmetic section for counting arrivals of the output pulse and appropriately calculating the counting rate per second of count with a sampling time T; a moving average value arithmetic section for calculating the moving average value, based on a plurality of counting rates per second of the count; a prediction arithmetic section for predicting the counting rate per minute of the present count, based on the present moving average value, previous moving average value; and counting rate per minute of the previous count using the equation: N 0 =60×(M 0 -M -1 )/Δt+N -1 , and a display section for displaying the predicted and calculated counting rate per minute of the present count. Here, N 0 is the counting rate per minute of the present count, N -1 is the counting rate per minute of the previous count, M 0 is a present moving average value, M -1 is a previous moving average value, and Δt is sampling time. COPYRIGHT: (C)2010,JPO&INPIT
    • 要解决的问题:提供一种用于预测,计算和显示辐射剂量测量装置的最终响应值的辐射剂量测量方法,而不必等待经过时间常数,并提供预测对应 型辐射剂量测量装置。 解决方案:该辐射剂量测量装置包括用于由辐射入射产生输出脉冲的输出部分; 计数速率运算部,用于计数输出脉冲的到达,并以采样时间T适当地计算每秒计数的计数率; 移动平均值运算部,其基于所述计数的每秒的多个计数率来计算所述移动平均值; 一个预测运算部分,用于根据当前移动平均值预测当前计数的每分钟的计数率,该前移动平均值; 和使用以下等式的先前计数的每分钟的计数率:N 0 = 60×(M 0 -M SB> -1 )/Δt+ N -1 ,以及显示部,用于显示当前计数的每分钟的预测和计算的计数率。 这里,N 0 是当前计数的每分钟的计数率,N -1 是先前计数的计数速率/分钟, SB>是当前的移动平均值,M -1 是先前的移动平均值,Δt是采样时间。 版权所有(C)2010,JPO&INPIT
    • 9. 发明专利
    • Radiation measuring device using optical fiber
    • 使用光纤的辐射测量装置
    • JP2005241447A
    • 2005-09-08
    • JP2004051837
    • 2004-02-26
    • Japan Nuclear Cycle Development Inst States Of ProjectsOhyo Koken Kogyo Co Ltd応用光研工業株式会社核燃料サイクル開発機構
    • ITO YASUHISAISHIKAWA HISASHIMIYAKE TOSHIOSAWADA TETSUO
    • G01T1/20G01T1/00
    • G01T1/2002
    • PROBLEM TO BE SOLVED: To measure surface contamination of a narrow part, a pipe or the like by narrowing and lengthening/thinning.
      SOLUTION: A long and narrow plane-shaped radiation detection part 10 equipped with a scintillator and a radiation measuring part 12 equipped with a photomultiplier are constituted separately, and both parts are connected with a waveform conversion optical fiber cable 14. A measured signal (light signal) by α rays detected by the radiation detection part is transmitted to the radiation measuring part through an optical fiber. The radiation detection part is equipped with a light guide having a long and narrow shape, waveform conversion optical fibers of a plurality of pairs each of which comprises two optical fibers which are arranged close along the light guide, a scintillator layer and a shielding film, and is formed by enclosing each component by a shielding frame having a long and narrow architrave structure so that only the shielding film on the front is exposed, and by drawing the optical fiber to the outside by a cable provided with a shielding casing.
      COPYRIGHT: (C)2005,JPO&NCIPI
    • 要解决的问题:通过变窄和延长/变薄来测量窄部分,管子等的表面污染。 解决方案:配备有闪烁器和配备有光电倍增管的辐射测量部分12的长而窄的平面状辐射检测部分10分别构成,并且两部分都与波形转换光纤电缆14连接。测量 由辐射检测部检测出的α射线的信号(光信号)通过光纤传输到辐射测量部。 放射线检测部配备有长形状的导光体,多对的波形变换光纤,其中包括沿导光体配置的两根光纤,闪烁体层和屏蔽膜, 并且通过由具有长而窄的楣结构的屏蔽框架包围每个部件而形成,使得只有前面的屏蔽膜露出,并且通过设置有屏蔽壳体的电缆将光纤拉到外部。 版权所有(C)2005,JPO&NCIPI
    • 10. 发明专利
    • Crucible and method for manufacturing fluoride crystal
    • 用于制造氟化物晶体的可制造和方法
    • JP2005035825A
    • 2005-02-10
    • JP2003198983
    • 2003-07-18
    • Nikon CorpOhyo Koken Kogyo Co Ltd応用光研工業株式会社株式会社ニコン
    • KITAMURA IKUOTAKANO SHUICHI
    • C30B11/00C30B29/12
    • PROBLEM TO BE SOLVED: To provide a crucible and a method for stably manufacturing a fluoride crystal which realize manufacture of a high quality fluoride single crystal having high transmittance in the ultraviolet region or the vacuum ultraviolet region.
      SOLUTION: The crucible for manufacturing the fluoride crystal is used for manufacturing the crystal by melting a fluoride material and a fluorinating agent. The crucible is composed of a main part for containing the fluoride material and the fluorinating agent and a cap part for covering the main part, and the main part and the cap part can be fixed to each other. A pressure regulating mechanism for regulating the pressure in the crucible is provided in at least either one of the main part and the cap part.
      COPYRIGHT: (C)2005,JPO&NCIPI
    • 解决的问题:提供一种在紫外线区域或真空紫外线区域中实现高透光率的高品质氟化物单晶的制造的氟化物晶体的坩埚和稳定制造方法。 解决方案:用于制造氟化物晶体的坩埚用于通过熔化氟化物材料和氟化剂来制造晶体。 坩埚由用于容纳氟化物材料和氟化剂的主要部分和用于覆盖主要部分的盖部分组成,并且主体部分和盖部分可以彼此固定。 用于调节坩埚中的压力的​​压力调节机构设置在主要部分和帽部分中的至少一个中。 版权所有(C)2005,JPO&NCIPI