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1.Advanced peak detector automatic cutoff with MOSFET and linear current charges battery to 100% without overcharging.
高级检测器自动以切断功率管输出和线性电流保证电池能被100%充满而不会导致过冲。收藏指正
2.Thirdly, the improved circuit system is expounded, which includes peak detector circuit, Automatic Gain Control circuit based on AD603, and counting circuit based on CPLD. Finally, after design of the circuit and debugging of the software and hardware being finished, experiments of the peak detector circuit and AGC circuit have been carried out.
再次,对改进后的电路系统进行了详细的介绍,其中包括值运算电路、基于AD603的自动增益控制(AGC)电路和基于复杂可编程逻辑器件(CPLD)的计数电路等。收藏指正
3.Calculation and application of absolute full-energy peak efficiency for Ge(Li) detector-counted sample system
Ge(Li)探测器系统的绝对全能探测效率计算收藏指正
4.The Compton suppression factors (CSF) measured are about 2.3, 4.1 and 4.6 in the energy region of 100~300, 300~800 and 800~1100 keV respectively to γ?rays from a ????60?Co source. The peak?to?total ratio is about 37%(for the relative efficiency 30% HPGe detector). ?
测得60Coγ射线源的康普顿抑制系数在能区100~300、300~800、800~1100keV范围内分别为2.3、4.1和4.6,且总比为37%(对相对效率为30%的HPGe探测器)。收藏指正
5.The selected chromatographic conditions were as follows: SE _ 30 column(2 m×3.2 mm), chromosorb W AW DMCS support, column temperature 250 ℃, injection temperature 280 ℃, flame ionization detector temperature 280 ℃. The fenpropathrin was quantitatively determined by the area of the chromatographic peak.
选定的色谱条件为5 %SE_30柱(2m×3.2mm) ,载体ChromosorbWAWDMCS,柱温250℃ ,气化室温度280℃ ,FID温度280℃ ,面积定量;收藏指正
6.Based on the feature of capillary electrophoresis affected by more uncertain fac tors, Monte Carlo simulation was used to explore the influences of error factors, such as op eration parameters of charge-coupled device detector, sample injection, applied voltages,temperature etc. , on detected signal intensities, determination accurcy and precision. And the relative superiority of quantitative calculation methods of peak height and peak volume is compared.
根据毛细管电泳分离受不确定因素影响较多的特点,应用MonteCarlo模拟方法,探讨了电荷耦合器件检测器操作参数,进样、电压、温度等误差因素对检测信号强度、测定准确度和精密度的影响,比较了高和体积定量计算方法的相对优劣,对进一步开发和应用电荷耦合器件检测毛细管电泳技术有一定意义。收藏指正
7.The radiation of positron annihilation in two aluminum samples from different origins was measured with the Ge(Li) detector. Using the 482 keV γ peak of 181Hf as reference, the relative positions of the annihilation peak centers were repetitively determined, the precision of the determination reached ± 6 eV. The results show that the rest mass of electron in these two different aluminum samples is consistent on 10 eV level.
用Ge(Li)探测器测量正电子在两种不同来源的铝样品中的湮没辐射,以~181Hf的482keVγ,做为基准,重复测定湮没与基准的相对位置,精密度达到±6eV。 结果表明,在两种铝样品中的电子静止质量在10eV水平上是一致的。收藏指正
8.A prototype planar CZT detector with sensitive volume of φ8×1.7mm3 has been fabricated and got the gamma-ray spectrum of 241Am. At the 59.54keV peak the FWHM is 2.21keV,while no polarization is observed and stability is very satisfactory.
已制成φ8mm×1.7mm灵敏体积的CZT探测器,室温下对241Am 59.54keV能量的γ射线分辨率为2.21keV(FWHM),连续测量没有极化效应,并且具有很好的长期稳定性。收藏指正
9.With the thin (0.3μm) ion-implanted p-type outside contact, the detector is able to detect X and γ rays from 5ekV to 10 MeV. The sensitive volume of the detector is about 120cm3, its relative efficieccy 24.5% energy resolutioe2.13 keV and the peak to compton ratio is 48.3:1 at 1.33 MeV γ ray. The electronic noise is 1.28 keV.
探测器具有薄的(约0.3μm)离子注入p~+外接触,可探测0.005—10MeV的X和γ射线,并具有较高的耐辐射损伤性能,所研制成的探测器灵敏体积约120cm~3,对1.33MeVγ射线:相对效率为24.5%,能量分辨率为2.13keV,康比为48.3:1,电子学噪声为1.28keV。收藏指正
10.The volume of the Ge(Li)detector was 78cm~3.For γ-ray of the energy of 1332keV of ~(60)Co,the resolution of thespectrometer was about 2.4keV,the ratio of the peak to compton was 6.4without shielding,the relative efficiency was 16%,and for the γ-ray peakof ~(137)Cs the detective efficiency was 1.6%.
Ge(Li)探测器的体积为78cm~3,对~(60)Co 的1332keVγ射线的分辨率为2.42keV,不加任何屏蔽时康比为36.4,相对效率为16%,对~(187)Cs 点源γ射线全能的探测效率为1.6%。收藏指正
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