| 1. | Photoflash'bulbs which usually have a duration of about 20 milliseconds above half peak intensity can be used either singly or flashed in sequence .
光强能在大约20毫秒持续时间内保持在半峰值以上的闪光灯，既可用于单次闪光，也可用于连续闪光。 |
| 2. | Peak intensity estimated
最高强度估计 |
| 3. | Limit outdoor activity between 11 a . m . - 3 p . m . when suns is at its peak intensity
上午11点至下午3点是一天中最热的时段，不宜进行大量户外活动。 |
| 4. | Limit outdoor activity between 11 a . m . - 3 p . m . when suns is at its peak intensity . wear lightweight , loose - fitting clothing
上午11点至下午3点是一天中最热的时段，不宜进行大量户外活动。 |
| 5. | The angle ( in the plane through the beam axis ) over which the luminous intensity drops to a stated percentage of its peak intensity
在光束的轴面上，光强值降至其峰值某一比例时所对应的角度。 |
| 6. | The x - ray diffraction analysis shows films prepared by rf and ve have scattering peaks , however the peak intensity of pure cdte films prepared by css method is higher than ahead both
而且用css方法制备的cdte薄膜晶粒度大，薄膜晶形好。利用近距离升华技术在glass / ito基片上先后沉积cds 、 cdte膜，保证cds膜的厚度< 2000 |
| 7. | The results indicate that the peak intensity of transmission beam is limited , and the cross - section intensity distribution is approximately flat - topped super gaussian , which shows the optical limiting effect of sbs
结果表明，透射光束截面光强呈现出近似平顶的超高斯分布，光强峰值被限制，显示出受激布里渊散射的空间光限幅效应。 |
| 8. | 2 we studied the films with raman polarization spectrum . the peak intensity in the polarization spectrum of the films with basal plane not oriented on the substrate changes with the polarization condition
张生仅北京工业大学博士学位论文摘要2利用raman偏振光谱研究了薄膜的性质，对基面非平行衬底的取向， raman谱随偏振条件的不同而变化。 |
| 9. | This work was initiated to establish an in - situ xrd measuring system through which the variations of xrd peak intensities on the surfaces of plzt ferroelectrics with fatigue numbers during an electric process can be in - situ observed
本工作通过建立原位xrd观测系统，对电疲劳过程中plzt铁电陶瓷试样表面x射线衍射峰随疲劳次数的变化进行了原位观测。 |
| 10. | The results show that the peak intensity of super - gaussian optical pulse becomes higher at the beginning , and the tail experiences a process of strengthening , and then weakening , which are different from gaussian optical pulse
数值模拟的结果表明，超高斯脉冲的波形演变和高斯脉冲有所不同，不但峰值能量经历了一个上升的阶段，而且拖尾振荡在初始阶段也经历了一个增强减弱的过程。 |
