| 1. | We consider a particle travelling in a given direction, say the x-direction .
我们考虑一个粒子沿已知方向，例如X方向运动。 |
| 2. | The disturbances advances in the x-direction as a so-called surface or evanescent wave .
这个扰动作为一个所谓表面波或倏逝波沿着X方向行进。 |
| 3. | What states have a definite momentum in the x - direction , say
譬如说，什么样的态在x方向具有确定的动量值？ |
| 4. | We consider a particle travelling in a given direction , say the x - direction
我们考虑一个粒子沿已知方向，例如x方向运动。 |
| 5. | The disturbances advances in the x - direction as a so - called surface or evanescent wave
这个扰动作为一个所谓表面波或倏逝波沿着x方向行进。 |
| 6. | In addition to , the slab model influent the structure - torsion greater . ( 4 ) the stiffness in y - direction is nearly equal to that in x - direction
( 4 )结构的y向刚度略小于x向刚度，两方向刚度比较接近，整体性较好。 |
| 7. | We consider two situations : ( i ) the light is polarized in the z - direction ; ( perpendicular to the cross - section of the wire ) . ( ii ) the light is polarized in the x - direction ( parallel to the cross - section of the wire )
考虑了两种不同情况：辐射光沿阱线的轴线方向偏振( z方向) ；辐射光?河北师范大学硕士研究生学位论文平行于轴截面偏振(设为x方向) 。 |
| 8. | In the scheme of the vccc , we calculate the relationships between the distributions of the magnetic field along z - axis or x - direction and various parameters of the vccc , and obtain several fitting equations that can be used to describe the relationships mentioned above
在v -型载流导体方案中，首先计算了磁场在导引中心处沿z轴方向和x方向上的分布，分析了磁场空间分布与载流导体参数之间的关系，给出了几个拟合公式。 |
| 9. | It was based on the principle of laser confocal microscope . and the two - dimensional scanning configuration was adopted by the optical scanner and the telecentric linear imaging objective lens of large numerical aperture to realize x - direction ' s scanning , and the conventional mechanical method using linear driver and linear guide track to y - direction ' s . the experiment results indicate that the device can run smoothly and rapidly , be operated easily and detect fluorescence effectively
仪器基于激光共焦显微镜的理论，采用振镜和远心线性成像物镜实现x向扫描；精密导轨和步进电机实现y向扫描的检测仪，经验证，扫描仪具有快速、操作简单、检测芯片能力良好等特征，有望弥补市场的空缺。 |
| 10. | We consider two situations : ( i ) the light is polarized along the z - direction , in which case the first allowed dipole transition is to the first subband ( nx - 1 , ny = 1 ) ; ( ii ) the light is polarized along the x - direction ( paralleled to the transverse cross - section of the wire ) . the first allowed dipole transition is to the second subband nx = 2 relative to the x - direction and to the first subband nr = 1 relative to the y - direction of the wire
考虑了两种不同惰况：辐射光沿阶线的轴线偏振k方向x辐射光平行于轴截面偏振（设为二方向山偶极跃迁的选择定则使得体系从初态跃迁到末态分别为电于的第一于带和第二子带，二名的光电离0截面随光于能量的变化截然不同 |
