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gamma
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  γ
    MODEL FH 1906 LOW BACKGROUND GAMMA SCINTILLATION SPECTROMETER
    FH1906型低本底 γ 闪烁谱仪
短句来源
    The measurement of gamma radiation of ~(125)iodine by liquid scintillation counter
    液体闪烁测量~(125)Iγ射线方法的研究
短句来源
    TOTAL SPECTRUM ENERGY METHOD FOR MEASURING ENVIRONMENTAL GAMMA EXPOSURE RATE BY NaI(Tl)γSPECTROMETER
    用 NaI(TI)γ 谱仪测量环境 γ 照射量率的总谱能量法
短句来源
    PORTABLE SCINTILLATION X OR GAMMA DOSE RATE METERS, TYPE SG 101, FOR MEASURING ENVIRONMENTAL RADIATION
    用于环境X,γ辐射测量的SG 101型可携式闪烁剂量率仪
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    STUDIES AND PREPARATION OF ~(192)Ir GAMMA RADIOGRAPHY SOURCES
    ~(192)Ir γ照相源的研制
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  “gamma”译为未确定词的双语例句
    TPGD-1 Dynamic Gamma Densitometer
    TPGD-1动态Υ密度计
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    APPLICATION OF NEUTRON PROMPT GAMMA RAYS USING A Cf-252 NEUTRON SOURCE TO MULTIELEMENTS ANALYSIS
    ~(252)Cf瞬发中子活化多元素分析方法的研究
短句来源
    Problems for Measurements of EnvironmentaI Gamma Radiation Using G-M Counter Dose Rate Monitors
    G-M计数管剂量率仪用于环境辐射水平测量时的一些问题
短句来源
    ACCURACY OF MEASUREMENT OF NATURAL GAMMA RAY SPECTRA BY HD-8004 NaI(T1)GAMMA SPECTROMETER
    ACCURACY OF MEASUREMENT OF NATURAL GAMMA RAY SPECTRA BY HD-8004 NaI(T1)GAMMA SPECTROMETER
短句来源
    Wide Structure of High Energy Gamma Ray Spectrum in Spontaneous Fission of ̄(252)Cf
    Wide Structure of High Energy Gamma Ray Spectrum in Spontaneous Fission of~(252)Cf
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  gamma
It is also shown that on the nilmanifold $\Gamma\backslash (H^3\times H^3)$ the balanced condition is not stable under small deformations.
      
For $\gamma\in\mathbb{R}$ let $C(\gamma)$ be the set of all $f\in{\mathcal S}^\prime$ for which$\sum_{n=0}^{\infty}\,|(f,h_n)|\,(n+1)^{\gamma}>amp;lt;\infty$, where $(h_n)_{n=0,1,\dots}$ is the orthonormal base of Hermite functions.
      
We show that $C(\gamma)\subset S_0$ if and only if $\gamma\geq\frac{1}{4}$ and that $S_0\subset C(\gamma)$ if and only if $\gamma\leq{-}\frac{1}{4}$.
      
Using these results we give an explicit solution of the problem of optimal reconstruction of functions from Sobolev's classes $W^{\gamma}_{p}(M^{d})$ in $L_{q}(M^{d}), 1 \leq q \leq p \leq \infty$.
      
This result generalizes the characterization of Fourier series of distributions with a distributional point value given in [5] by $\lim_{x\rightarrow\infty}\sum_{-x\leq n\leq ax}a_{n}e^{inx_{0}}=\gamma\ (\mathrm{C},k)\,$.
      
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Thermoluminescent detector(TLD)is a new solid state dose meter.Inthis paper,we describe the application of CaSO_4(Tm)TLD to personal exposure,environmental monitering and gamma rays measurement in reactor.In addition,the compare of measurement values obtained by the CaSO_4(Tm),FT-301 andNYL-3 dose meters is given,we find that the results are approximate eachother.

热释光剂量计是一种新型的固体剂量计。本文介绍了 CaSO_4(Tm) 热释光剂量计在个人剂量、环境监测和堆内γ测量等方面的应用。文中给出了 CaSO_4(Tm)与 FJ-301、NYL-3剂量计的测值比较,结果符合得很好。

The heat generation of pressure vessel and tube under gamma irradiat-ion yields thermal stress with bulk heat source when the outside surface ofthe hollow cylinder is adiabatic,the solution of thermal stress has beengiven by Takenouchi.When the hollow cylinder is cooling both inside andoutside,the computation of thermal stress is considered in this paper.

反应堆或辐照装置的压力壳和压力管,由于吸收γ射线而发热,形成有内热源的热应力问题。当圆筒外壁绝热时,热应力的解已由竹内给出。本文给出在圆筒内外同时冷却时的热应力计算方法。

This computer code uses the method of steepest descent to minimize laminatedshield weight.It is applicable to slab,cylinder and sphere geometries.The neu-tron flux distribution through the shield is obtained by a few group diffusionequations;the gamma ray attenuation is treated in the point kernel integral me-thod.The optimization is performed for Pb-H_2O and Fe-H_2O shielding configu-rations.

本程序使用最速下降法寻求分层屏蔽重量最小化,适用于平板,圆柱和球形几何。中子通量分布用少群扩散方程得到;γ射线的处理用点核积分方法。对铅-水和铁-水屏蔽结构进行了最佳化计算。

 
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