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gas target
相关语句
  气体靶
     The Optimization Analysis and Design of Gas Target Thickness of HT-7 Neutral Beam Injection System
     HT-7中性束注入器气体靶厚度优化分析与设计
短句来源
     And the spectra from the laser plasma soft X_ray source with copper target and O 2,Kr gas target are measured in 8~30nm region, respectively by means of the above_mentioned way.
     使用这种方法测量了铜靶激光等离子体光源和氧、氪气体靶激光等离子体软X射线源在 8~ 30nm波段的光谱
短句来源
     A tritium gas target was built and employed in neutron physics experiments at HI 13 tandem accelerator.
     在HI-13串列加速器上建立了我国第一台氚气体靶装置。
短句来源
     The article primary introduces composing of HT-7 Neutral Beam Injection (NBI) system, then mainly analyzes gas target thickness, that is pressure distribution of neutralizer gas cell, one of factors which affect heating efficiency of NBI.
     本文首先介绍了HT-7中性束注入(NBI)加热系统的组成,然后对影响中性束注入加热效率因素之一的气体靶厚度即中性化室的压力分布进行了重点分析。
短句来源
     Experimental Investigation of Laser Plasma Soft X-ray Source with Gas Target
     气体靶激光等离子体软X-射线源实验研究
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  “gas target”译为未确定词的双语例句
     It is shown that an 123I yield of 5.92MBq can be obtained or optimum retrieving time of 5.26h, with a 3MPa 124Xe gas target and 3h borobardment time.
     并给出~(124)Xe高压气靶为3MPa,当照射3h,在最佳回收时间5.26h回收氙气,可获得123I的活度约5.92MBq。
短句来源
     In static gas target, the 5th -17th (40-160 nm) high harmonic generation soft X-ray laser radiation has been obtained using linearly-polarized Ti: sapphire ultra-short laser pulses( central wavelength is 795 nm, pulse duration is 105 fs, repetition rate is 10 Hz and one pulse energy is 50 mj) .
     在静态气室中,利用线偏振的掺钛蓝宝石(Ti:sapphire)超短脉冲激光(中心波长795nm,脉宽105fs,重复频率10Hz,单脉冲能量50mJ),获得氙气中5~17次(40~160nm)谐波的软X射线激光辐射。
短句来源
     The paper introduces the methods for making some special targets including self-supporting Bi targets of 70 mg/cm2, Mo window foils for gas target, self-supporting Sc targets of 0. 015 mg/cm2, (CD2)n targets and self-supporting Co targets of 0. 08 mg/cm2.
     文章介绍了几种特殊靶的制备,包括70mg·Cm-2的自支撑Bi靶、Mo封窗膜、15—50μg·Cm-2的自支撑Sc靶、(CD2)n靶和70μg·cm-2的自支撑Co靶。
短句来源
     By using a gridded ionization chamber, the differential cross sections and angle integrated cross sections for the 6Li(n,t) 4He reaction were measured at neutron energies of 3.67 and 4.42MeV. The neutrons were produced through D(d,n) 3He reaction by a deuteron gas target.
     用屏栅电离室对 3.6 7MeV与 4 .4 2MeV中子6Li(n ,t) 4He反应微分截面进行了测量。
短句来源
     SYUDY OF THE DYNAMIC GAS TARGET DIVERTOR IN THE FEB-E
     FEB-E动态气靶偏滤器的研究
短句来源
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  相似匹配句对
     N TARGET
     命中目标
短句来源
     GAS SENSORS IN TARGET DETECTION
     气体传感器在目标探测中的应用研究
短句来源
     SYUDY OF THE DYNAMIC GAS TARGET DIVERTOR IN THE FEB-E
     FEB-E动态气靶偏滤器的研究
短句来源
     Gas Analyses
     气体分析
短句来源
     Gas Station
     加油站
短句来源
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  gas target
The PISCES-A linear plasma device (n ≤ 3 × 1019 m-3, kTe ≤ 20 eV) has been used to simulate a gas target divertor.
      
Impurity Transport in a Simulated Gas Target Divertor
      
The protons were scattered on A gas target at pressures from 520 to 620 mm Hg.
      
A model for production of episodic γ-ray event at interaction of a moving gas target with, a beam of relativistic particles is proposed.
      
The neutron beam was produced at the TANDEM accelerator of NCSR "Demokritos" by the 2H(d,n)3He reaction, using a deuterium gas target.
      
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The cross sections of deutron-deutron reaction for deutron energy from 15 keV to 150 keV and of deutron-tritium reaction for deutron energy from 13.8 keV to 114.3 keV were measured by the process of passing a deutron and tritium beam into a gas target formed by a differential pumping system and two capillary pipes. Experiments in two steps-angular distribution measurement and absolute differential cross-section measurement-were performed at 3 Cockcroft-Walton generators with terminal voltages of 50 kV,...

The cross sections of deutron-deutron reaction for deutron energy from 15 keV to 150 keV and of deutron-tritium reaction for deutron energy from 13.8 keV to 114.3 keV were measured by the process of passing a deutron and tritium beam into a gas target formed by a differential pumping system and two capillary pipes. Experiments in two steps-angular distribution measurement and absolute differential cross-section measurement-were performed at 3 Cockcroft-Walton generators with terminal voltages of 50 kV, 150 kV and 300 kV. Emperical fit of D-D reaction data to Gamow formulae and comparison of D-T reaction data with BWE theory were given.

采用无窗气体靶技术测量了15—150keV的氘-氘以及13.8—114.3keV的氘-氚反应截面,误差≤±5.1%。实验是分别在50kV、150kV、300kV三台倍加器上进行的。测量分绝对微分截面与相对微分截面测量两步进行。在完成测量数据的实验过程中,相应地发展了氚操作技术与加速氘、束流热测法(量热器)以及对气体的压力、温度、纯度绝对值测量等方面的技术。

Calculation and experimental results of the gas flow rates and pressures in the discharge chamber and neutralize, gas target thickness in the neutralize, neutralization efficiency, reionization and heat load in the TEXTOR beam lines and the power into TEXTOR are presented.

本文给出TEXTOR束线中放电室送气量和气压、中性化室送气量和气压、中性化室气体靶厚、中性化转换效率、再电离、热负荷、注入TEXTOR功率和粒子数的计算和实验结果。

A multi-detector fast neutron time of flight spectrometer is built at HI-13 tandem accelerator and compared with existing ones. The spectrometer will be used for measurements of fast neutron scattering angular distributions and double differential cross sections of secondary neutrons as well as charged particle induced neutron emission spectrum study. Main parts of the spectrometer (including beam pick-off system, deuterium gas target, neutron detector and electronics) are described briefly. The performance...

A multi-detector fast neutron time of flight spectrometer is built at HI-13 tandem accelerator and compared with existing ones. The spectrometer will be used for measurements of fast neutron scattering angular distributions and double differential cross sections of secondary neutrons as well as charged particle induced neutron emission spectrum study. Main parts of the spectrometer (including beam pick-off system, deuterium gas target, neutron detector and electronics) are described briefly. The performance of the spectrometer and some applications in fast neutron experiment are also depicted.

描述了一台串列加速器HI-13上的多探测器快中子飞行时间谱仪,并与国际上同类谱仪进行了比较。本谱仪主要用于能量大于8 MeV的快中子散射实验、次级中子双微分截面及带电粒子引起的出射中子能谱的测量。简要介绍了谱仪各主要部分(包括零信号拾取筒、氘气体靶、探测器、电子学等)的结构和特性及其在快中子实验中的应用。

 
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