The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,映了分布决等色线、振幅分布决消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固和流中的，即慢纵波在流中振幅大，而在固中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝热电子跃迁过程．导出并求解了跃迁几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳定的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,反映了相位分布决定等色线、振幅分布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中振幅大，而在固相中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝热电子程．导出并求解了几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳定的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,反映了相位分布决定等色线、振幅分布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中振幅大，而在固相中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝跃迁过程．导出并求解了跃迁几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

光偏仪(DOAP)是一种高速测量光波偏态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳定的波节区而轮廓线则描绘出等的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,反映了相位布决定等色线、布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中大，而在固相中的较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描热电子跃迁过程．导出并求解了跃迁几率的运动方程，该方程正确描了共态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分幅光(DOAP)是一种高速测量光波态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受转的或稳定的波节区而轮廓线则描绘出等幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的光干图,反映了相位分布决定等色线、幅分布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中幅大，而在固相中的幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力法描写非绝热电子跃迁过程．导出并求解了跃迁几率幅的运动程，该程正确描写了共态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳定的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,反映了相位分布决定等色线、振幅分布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中振幅大，而在固相中的振幅。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

量于力学方法描写非绝热电子跃迁过程．导出并求解了跃迁几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳定的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,反映了相位分布决定等色线、振幅分布决定消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中振幅大，而在固相中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝热电过程．导出并求解了几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的或稳的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针取向的双轴晶体,计算了完整的偏光干图,反映了相位分等色线、振幅分消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固相和流相中的相位相反，即慢纵波在流相中振幅大，而在固相中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝热电子跃迁过程．导出并求解了跃迁几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。

The division-of-amplitude photopolarimeter (DOAP) is a sensor that can rapidly determine the polarization state of the incident light.

分振幅光偏振仪(DOAP)是一种高速测量光波偏振态的传感器。

Bright areas reveal undeflected or stationary nodal regions while contour lines trace out areas of constant vibrational amplitude.

亮区表示未受偏转的的波节区而轮廓线则描绘出等振幅的区域。

The conoscopic interference patterns of crystals are calculated for any orientation biaxial crystal, which include information of isochromatic curve and isogyre.

针对任意取向的双轴晶体,计算了完整的偏光干图,映了分布决等色线、振幅分布决消光影的规律。

And the special phenomena such as the S wave splitting, the blind points of the S wave splitting and wavefront triplication are dearly observed.

而慢纵波在固和流中的，即慢纵波在流中振幅大，而在固中的振幅较小。

Using the guantum mechanics method to describe the electronically nonadiabatic transition, the equation of the motion of the nonadiabatic transition probability amplitutes have been derived.

用量于力学方法描写非绝热电子跃迁过程．导出并求解了跃迁几率振幅的运动方程，该方程正确描写了共振态的存在和驰豫现象。