| 1. | At the same time broaden the spectrum as result of energy loss fluctuations .
与此同时，电子谱由于能量损失的涨落而展宽。 |
| 2. | The shape of the electron spectrum in beta decay is not dominated by properties of the matrix element .
衰变的电子谱的形状不取决于矩阵元的性质。 |
| 3. | Aes analysis of optoelectronic materials
光电材料的俄歇电子谱分析 |
| 4. | Angle resolved electron spectroscopy
角分辨电子谱法 |
| 5. | Standard guide for identifying chemical effects and matrix effects in auger electron spectroscopy
在俄歇电子谱法中测定化学效应和基质效应 |
| 6. | The gamma - ray leakage energy spectra s are resolved from the compton electron recoil spectra
测量得到的康普顿反冲电子谱通过解逆矩阵得到射线能谱s 。 |
| 7. | Measurements of compton recoil electron spectra caused by the gamma ray are detected by a nominal 5 . 08cm - diam 5 . 08cm - long bc - 501a scintillator detector
Bc - 501a液体闪烁探测器用于测量射线产生的康普顿反冲电子谱。 |
| 8. | Angular distribution and energy spectrum of the hot electrons emission resulted from the interaction of the us - ui laser pulse with plasma are measured with the calibrated lif tlds , and the yield of the hot electrons is consistent with the results of the other experiments
采用这样标定的l正tlds作为电子谱仪的探测元件，所测量的超热电子产额与国外同类实验测量的超热电子产额较好地一致。 |
| 9. | In the investigation of the interaction of the us - ui laser pulse with the plasma , a standard - ray source is firstly used to absolutely calibrate lif mermc - luminescence dosimeters ( tlds ) , and the dosimeter are employed as the angular distribution spectrometer and the energy spectrum spectrometer of the hot electrons
在超短超强激光等离子体相互作用的研究中，首次采用137cs邓标准源对lif热释光探测器( tlds )进行了绝对标定。并以此作为电子角分布仪和电子谱仪的探测元件，研究了超短超强激光与等离子体相互作用中超热电子发射的角分布和能量分布。 |
| 10. | At first , measuring the electron recoil spectra of target room gamma ray . through the resolution of spectra we get the gamma ray spectra caused by target room . then we transform it to the zero point , the place of neutron source , and calculate the leakage gamma ray spectra t from iron sphere caused by target room gamma ray by mcnp program
靶室产生的射线本底，通过实验测量和模拟计算相结合的方法加以扣除，首先测量靶室产生的射线康普顿反冲电子谱，解谱得到靶室泄漏谱，将所解得的靶室泄漏谱归一到原点，即中子源处，利用mcnp蒙卡程序输运计算靶室射线穿透铁球后所泄漏的能谱，最后从d ? t中子穿透铁球伴生射线泄漏能谱s中扣除。 |
