| 1. | Data acquisition system based on vxi for icf
实验中超热电子测量的数据采集系统 |
| 2. | Influnce of au cone on distribution of forward hot electrons
金锥对靶背向超热电子分布的影响 |
| 3. | The spectrum can be fitted by maxwellian distribution , the hot electron temperature given by the slope is 67kev
用maxwellian分布拟合能谱，超热电子温度为67kev 。 |
| 4. | Influence of laser incidence angle on hot electrons generated in the interaction of ultrashort intense laser pulses with foil target
激光入射角对靶面方向超热电子发射的影响 |
| 5. | These emission peaks are located in the directions of the specular reflection of laser , the target normal and the back - reflection of laser respectively
这些超热电子发射峰分别沿着激光反射方向、靶法线方向和激光背反射方向。 |
| 6. | As our best known , this is the first experimental measurement of so high hot electron temperature at moderated intensity , pre - pulse free condition
据我们所知，这是第一次报道在10 ~ ( 16 ) w cm ~ 2 、无预脉冲条件下，实验测量到这么高的超热电子温度。 |
| 7. | In this experiment the ponder - motive force can compete with plasma thermal pressure , which is estimated by theory and confirmed by frequency shift measured in reflected light of uv laser
从真空吸收给出的超热电子温度的定标率来看，实验中测量得到的超热电子温度是合理的。 |
| 8. | In the experiment of the angular distribution of the hot electrons emission , three - peaks and double - peaks emission of the hot electrons resulted from the multi - acceleration mechanisms are observed in our experiments
在超热电子发射的角分布实验研究中，发现由几种加速机制所支配的超热电子的三峰发射和双峰发射。 |
| 9. | From the scaling law about hot electron temperature given by vh model , the hot electron measured by experiment was reasonable , the temperature was higher than the temperature given by resonant absorption scaling law
真空吸收是产生高能超热电子的主导过程，从真空吸收给出的超热电子温度定标率来看，实验中测量得到的超热电子温度是合理的。 |
| 10. | 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。 |
