拉盖尔高斯涡旋光束的传输  

Propagation of Laguerre-Gaussian vortex beam

作　　者：丁攀峰[1] 蒲继雄[1] 

机构地区：[1]华侨大学信息科学与工程学院,泉州362021

出　　处：《物理学报》2011年第9期338-342,共5页Acta Physica Sinica

基　　金：福建省自然科学基金(批准号:A0810012);国家自然科学基金培育计划项目(批准号:JB-ZR1126)资助的课题~~

摘　　要：针对拉盖尔高斯涡旋光束,推导了其传输后目标平面上光电场的解析表达式,理论研究表明,传输一段距离后,对于拉盖尔高斯光束的光斑大小的描述,高斯光斑尺寸已经不再适用.如果采用光强最亮处的半径来表示目标平面上的光斑大小则比较方便.除了传输中的衍射导致光束展宽以外,横截面上光束的相位分布也发生了独特的变化.等相位线由原来的射线转化为弧线,拓扑电荷数为正时,弧线朝顺时针方向弯曲,拓扑电荷数为负时,弧线朝逆时针方向弯曲.For Laguerre Gaussian vortex beam, the analytical expression of the electric field is derived in the observation plane after propagation. Theoretical analysis shows that the definition of Gaussian beam is unsuitable to describing the size of the laguerre Gaussian vortex beam while propagation. It is more convenient that the radius of the point where intensity is maximum is used to define the vortex beam after propagation. Besides the beam broadening effect induced by diffraction, phase distribution exhibits special change in the observation plane. Isophase line changes from radial to arc. If the topological charge of the vortex beam is positive, the isophase line will bend clockwise after propagation; if the topological charge of the vortex beam is negative, the isophase line will bend anticlockwise.

关 键 词：涡旋光束 传输 光斑尺寸 相位分布 

分 类 号：O436[机械工程—光学工程]