物理学报
物理學報
물이학보
2015年
8期
084210-1-084210-7
,共1页
宋洪胜%刘桂媛%张宁玉%庄桥%程传福
宋洪勝%劉桂媛%張寧玉%莊橋%程傳福
송홍성%류계원%장저옥%장교%정전복
相位奇异%散斑%离心率%统计规律
相位奇異%散斑%離心率%統計規律
상위기이%산반%리심솔%통계규률
phase singularity%speckle%eccentricity%statistical property
利用散斑场和参考光的干涉提取散斑场复振幅和相位,研究了不同散射角下散斑场相位的分布规律以及相位奇异处光波复振幅实部零值线和虚部零值线夹角、光强等值线离心率的统计特性。在大散射角散斑中发现了一种新的相位奇异现象,即相位奇异线;研究了相位在跨越奇异线时的突变规律及涡旋状相位的分布特征,发现在相位奇异线处存在着呈双曲线或抛物线状的光强等值线。
利用散斑場和參攷光的榦涉提取散斑場複振幅和相位,研究瞭不同散射角下散斑場相位的分佈規律以及相位奇異處光波複振幅實部零值線和虛部零值線夾角、光彊等值線離心率的統計特性。在大散射角散斑中髮現瞭一種新的相位奇異現象,即相位奇異線;研究瞭相位在跨越奇異線時的突變規律及渦鏇狀相位的分佈特徵,髮現在相位奇異線處存在著呈雙麯線或拋物線狀的光彊等值線。
이용산반장화삼고광적간섭제취산반장복진폭화상위,연구료불동산사각하산반장상위적분포규률이급상위기이처광파복진폭실부령치선화허부령치선협각、광강등치선리심솔적통계특성。재대산사각산반중발현료일충신적상위기이현상,즉상위기이선;연구료상위재과월기이선시적돌변규률급와선상상위적분포특정,발현재상위기이선처존재착정쌍곡선혹포물선상적광강등치선。
Based on the interference patterns of the speckle field and the reference beam recorded by the charge-coupled device, and the digital Fourier transform technique, the complex amplitudes and phases of speckle field produced at different scattering angles are extracted. The phase distribution and the statistical properties at the singular point, such as the angle between two zero-contour lines of real part and imaginary part of the complex amplitude, the eccentricity of the intensity contours, etc. are studied. We find that there are some special properties of phase singularity when the scattering angle is large enough. With the increase of the scattering angle, great changes have taken place in the spatial distributions of the amplitude and the phase, and the probability of the angle between two zero-contour lines of real part and imaginary part is close to a smaller value, and the average eccentricity of the intensity contours around the phase singularity gradually increase. Moreover, the most interesting thing is that the eccentricity is probably greater than 1 in large anger scattering. The phase singular line as a new kind of phase singularity is found at a large scattering angle;the phase mutation rules and the vortex distribution characteristics of the phase on both sides of the phase singular line are investigated, and the hyperbolic or parabolic shape intensity contour around the phase singular line is found.