孔径

Meanwhile, we carried out the Z-scan experiments of pure CS2 to confirm the results of numerical simulation in the case of large nonlinear phase shift induced by a picosecond pulsed laser.

随着透过光阑孔径的增加，Z扫描曲线峰的变化要明显快于谷的变化，而且在谷明显存在的情况下，峰很快消失。

In simulations, the layered pillared nano-material is represented by the model with uniform distribution of pillars between two solid walls.

根据常温下甲烷在活性炭中的吸附实验数据，首次用GCMC和统计积分方程结合的方法求解了活性炭的孔径分布。

Adsorption of CCl〓 in slit pores and pillared nano-materials at ambient temperature T=300K was simulated.

模拟了超临界甲烷在不同孔径和不同孔率的层柱材料中吸附。

Then, an effective model is proposed by introducing the wall-fluid binary interaction parameters k〓 to the layered pillared pore model.

得到活性炭的孔径分布之后，使用该活性炭模型预测了常温下四氯化碳的吸附回收情况。

Finally the pipelining architecture and simulation result are proposed.

最后给出了相应的子孔径成像流水实现结构和仿真结果。

They are exposure, refraction, plane of focus, angle of view and aperture.

他们曝光，折射，平面透视视角和孔径。

Considering the ionospheric refractive index in geomagnetic field, the radiowave polarization plane rotation has been calculated. For linear frequency modulation pulse signal, the expression of Doppler shift error due to ionospheric dispersion characteristics is derived.

本文还计算了考虑地磁场时电离层双折射指数特性引起的电波极化面旋转角，推导出对于线性调频脉冲信号电离层介质色散特性引起的合成孔径时间内多普勒频移误差的表达式。

The result of this paper is popular for different kind of space-borne SAR system.

所得结果普遍适用于不同轨道和雷达参数的星载合成孔径雷达系统。

More influence of WHSV on activity was observed over smaller pore catalysts.

3催化剂的有效孔径越大，醚化活性受空速的影响越小。

A new method was put forward for measuring the pore size and its distribution.

为膜孔径大小及其分布的测定提供了一条新的思路。

The split between the two groups can hardly be papered over.

这两个团体间的分歧难以掩饰。

This approach not only encourages a greater number of responses, but minimizes the likelihood of stale groupthink.

这种做法不仅鼓励了更多的反应，而且减少跟风的可能性。