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    • 63. 发明授权
    • Method and apparatus for using non-linear spectral fitting procedures on
gamma-ray spectral data
    • 在伽马射线谱数据上使用非线性光谱拟合程序的方法和装置
    • US5369578A
    • 1994-11-29
    • US64622
    • 1993-05-20
    • Bradley A. RoscoeChristian Stoller
    • Bradley A. RoscoeChristian Stoller
    • G01V5/06G01V5/10G06F15/21
    • G01V5/101G01V5/06
    • A method and an apparatus for decomposing a gamma spectrum representative of an unknown material for determining the contribution of each constituent postulated to constitute the material, wherein an energy spectrum of the gamma rays issued from the material is formed, as well as a composite spectrum made up of individual standard spectra of the postulated constituents and comprising elemental yields being representative of the proportion of the corresponding constituents; the best fit between the measured spectrum and the composite spectrum is determined by modifying simultaneously at least one elemental yield and at least one parameter representative of the conditions under which the measured spectrum and the composite spectrum have been obtained. The best fit may be based on any non linear least squares search for a global minimum of X.sup.2 =(S Y-U).sup.T W(S Y-U), where "U" is a matrix representing the measured spectrum, "S" is a matrix representing the composite spectrum, "Y" is a matrix representative of the elemental yields and "W" is a weight matrix. The non linear fitting method used may be e.g. a gradient search or the Marquardt method.
    • 一种用于分解表示未知材料的伽马光谱的方法和装置,用于确定假定构成材料的每个组成部分的贡献,其中形成从材料发出的伽马射线的能谱以及形成的复合光谱 假定的成分的单个标准光谱的单位,并且包括代表相应成分的比例的元素产率; 测量光谱和复合光谱之间的最佳拟合通过同时修改至少一个元素产量和至少一个代表所获得的测量光谱和复合光谱条件的参数来确定。 最佳拟合可以基于任何非线性最小二乘搜索全局最小值X2 =(S YU)TW(S YU),其中“U”是表示测量光谱的矩阵,“S”是表示 复合光谱,“Y”是表示元素产量的矩阵,“W”是权重矩阵。 所使用的非线性拟合方法可以是例如。 梯度搜索或Marquardt方法。
    • 64. 发明授权
    • Method and apparatus for determining the respective contributions of
borehole and earth formation in gamma ray spectroscopy
    • 用于确定伽马射线光谱法中钻孔和地层各自贡献的方法和装置
    • US5105080A
    • 1992-04-14
    • US679468
    • 1991-04-02
    • Christian StollerRobert A. Adolph
    • Christian StollerRobert A. Adolph
    • G01V5/10
    • G01V5/104G01V5/101
    • A apparatus and an apparatus for determining the respective contributions in spectroscopy measurements of the borehole and the earth formations surrounding the borehole, derived from the detection of gamma rays resulting from the collisions of neutrons with atoms of the formation or the borehole. From gamma rays from a near and far detector, and established, at each depth, responses (e.g. elemental yields) representative of the values of an unknown in the borehole and in the formation. The far detector response is plotted against the near detector response. From the plot and from known conditions of the detection, is derived a closed curve characteristic of the relative contributions of the borehole and the formation in the responses. For each depth, the respective values of the unknown are derived from the position on the plot of the couple of responses for that depth, with respect to the closed curve. For instance, on a plot of C/(C+O) yields, the curve is a parallelogram two concurrent sides of which form a coordinate system; the coordinates of each response corresponds to the values of the unknown respectively for the formation and the borehole.
    • 一种装置和装置,用于确定由探测由中子与地层原子或井眼碰撞而产生的伽马射线的钻孔周围的钻孔和地层的光谱测量中的各自贡献。 来自近距离和远距离探测器的伽马射线,并且在每个深度处确定代表井眼和地层中未知物的值的响应(例如元素产量)。 远检测器响应相对于近检测器响应绘制。 从图的情况和已知的检测条件,得出了井眼的相对贡献和响应中的形成的闭合曲线特征。 对于每个深度,未知的相应值来自相对于闭合曲线的该深度的响应对的图上的位置。 例如,在C /(C + O)产量的曲线上,曲线是平行四边形,两个并列的边形成一个坐标系; 每个响应的坐标分别对应于地层和钻孔的未知值。
    • 70. 发明申请
    • NEUTRON DETECTION BASED ON A BORON SHIELDED GAMMA DETECTOR
    • 基于BORON屏蔽GAMMA检测器的中子检测
    • US20130206972A1
    • 2013-08-15
    • US13807694
    • 2011-06-26
    • Tong ZhouDavid RoseSicco BeekmanChristian Stoller
    • Tong ZhouDavid RoseSicco BeekmanChristian Stoller
    • G01T3/06G01T1/20G01V11/00
    • G01T3/06G01T1/20G01V5/104G01V11/00
    • A method is provided to detect neutrons using a boron-shielded gamma-ray detector, which will detect the 0.48-MeV prompt gamma ray due to the 10B (n,α)7Li reaction. The gamma ray detector can be a proportional gas counter, a scintillation based detector, or a semiconductor detector. Monoenergetic prompt gammas will produce a sharp peak in the pulse height spectrum of a gamma-ray spectroscopy detector. By surrounding a gamma detector with a layer containing 10B, we can measure the gamma signal and neutron signal at the same time and at the same physical location in an instrument. The approach can be used to measure neutron porosity simultaneous with gamma-ray counting or spectroscopy at the same location as long as the 0.48-keV gamma-ray from the neutron reaction does not interfere with the gamma-ray measurement.
    • 提供了一种使用硼屏蔽伽马射线检测器检测中子的方法,该检测器将检测由于10B(n,α)7Li反应而导致的0.48-MeV提示γ射线。 γ射线检测器可以是比例气体计数器,基于闪烁的检测器或半导体检测器。 单能提示伽马将在伽马射线光谱检测器的脉冲高度谱中产生尖锐的峰值。 通过围绕包含10B的层的伽马检测器,我们可以在仪器的同一时间和相同的物理位置测量伽马信号和中子信号。 只要来自中子反应的0.48keV伽马射线不干扰伽马射线测量,该方法可以用于在相同位置处与伽马射线计数或光谱同时测量中子孔隙。