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摘要:
为了产生轴向双焦点中空环形光斑，基于矢量衍射积分得出的环带半径公式，设计产生了呈环带分布的轴向双焦点的螺旋相位，并研究了这种螺旋相位在高数值孔径物镜聚焦区域的光斑特性。首先，给出了线偏振以及圆偏振的涡旋光束在高数值孔径物镜聚焦条件下的积分表达式。然后，利用此积分表达式数值模拟了线偏振光与圆偏振光在不同轴向偏移距离及螺旋拓扑荷值时的聚焦光场分布。最后，将轴向双焦点螺旋相位加载到纯相位空间光调制器上，分别对圆偏振光与线偏振光入射进行实验研究。线偏振光入射时，实验产生了拓扑荷为1且轴向距离为±10 μm、±15 μm的双聚焦环形光斑；圆偏振光入射时，产生了轴向距离为±20 μm且拓扑荷为1到4时的双聚焦环形光斑。数值模拟与实验结果表明：圆偏振光与线偏振光经此螺旋相位调制后，在紧聚焦区域可产生轴向距离与暗斑大小可调的中空环形双焦点；圆偏振光较线偏振光产生的空心光斑光强分布更均匀，呈圆对称分布。此轴向双焦点螺旋相位有望在光学微操控、双光束超分辨纳米光刻以及STED显微成像方面获得一定的应用。
Abstract:In order to generate double doughnut-shaped focal spots at adjustable positions along the axial direction, a vortex phase zone plate based on a formula of annular radius derived from vector diffraction integral was designed. The focusing properties of the modulated vortex phase zone plate were further investigated in a tightly focused system. First, integral formulas of linearly and circularly polarized vortex beams were calculated under high NA focusing conditions. Then, the intensity distributions of linearly and circularly polarized vortex beams in a high NA focusing system were simulated by integral formulas with various axial shifting distances and topological charges. Finally, the corresponding experimental results of linearly and circularly polarized light were also given, utilizing a spatial light modulator loaded on double doughnut-shaped phase patterns. The double doughnut-shaped focal spots with a topological charge of 1 and axial distances of ±10 μm and ±15 μm were produced when the incident light was linearly polarized. As well as the double doughnut-shaped focal spots with axial distances of ±20 μm, topological charges of 1−4 were also produced when the incident light was circularly polarized. The simulated and experimental results demonstrated that two doughnut-shape focal spots with controllable axial shifting distances and dark spot sizes could be produced in the tight focusing region of a high NA objective when it is modulated by the vortex phase zone plate. This kind of vortex phase zone plate could be applied in the field of optical micromanipulation, two-beam super-resolution nanolithography, and Stimulated-Emission-Depletion (STED) fluorescence microscopy.
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图 2线偏振光入射时的数值模拟结果，其中拓扑荷n=1，数值孔径NA=0.85。涡旋相位图中的轴向偏移距离分布为：(a) |Δz|=10 μm，(c) |Δz|=15 μm，(e) |Δz|=20 μm。(b)、 (d)、 (f)分别为对应的yz截面光强分布图
Figure 2.The simulation results of incident linearly polarized light withn=1 andNA=0.85. The axial shift distances of the vortex phase zone plate are: (a) |Δz|=10 μm; (c) |Δz|=15 μm; (e) |Δz| = 20 μm. (b), (d) and (f) are the correspondingyzcross-section distributions of the total intensity in (a), (b) and (c), respectively
图 3线偏振光 (a)~(c)和圆偏振光 (d)~(f)入射时的数值模拟结果，其中拓扑荷n= 1，轴向偏移距离|Δz|=10 μm，数值孔径NA=0.85。(a)、 (d)为聚焦光斑在xy截面上的光强分布； (b)、 (e)为聚焦光斑在一维x轴和y轴方向上的归一化光强分布； (c)、 (f)为聚焦场的三维强度等值面分布图，其中的等值面为I1= 0.5Imax，I2= 0.3Imax
Figure 3.The simulation results of linearly polarized light (a)−(c) and circularly polarized light (d)−(f) withn=1, |Δz|=10 μm andNA=0.85. (a), (d) are thexycross-section distributions of total intensity; (b), (e) are the normalized intensity alongxandyaxis directions; (c), (f) are the 3D iso-surface plots of the total intensity withI1= 0.5Imax,I2= 0.3Imax
图 4圆偏振光入射时的相位分布图 (a)~(d) 及其对应的紧聚焦xy截面的光场强度分布 (e)~(h)。其中，数值孔径NA=0.85，|Δz|=20 μm涡旋波带片的拓扑荷数： (a)， (e)n=1；(b)， (f)n=2；(c)， (g)n=3；(d)， (h)n=4
Figure 4.(a)−(d) are the phase distributions of vortex phase zone plate, (e)−(h) are the correspondingxycross-section distributions of light intensity in the tight focusing field illuminated by circularly polarized light, in whichNA=0.85, |Δz|=20 μm and the topology charge: (a), (e)n=1; (b), (f)n=2; (c), (g)n=3; (d), (h)n=4
图 5实验光路示意图。其中：PHF为针孔滤波器；CL为准直镜；BS为分束棱镜；P为偏振片；SLM为空间光调制器；PM为平面反射镜
Figure 5.Schematic diagram of the optical path in experiment, where PHF is a pin hole filter, CL is a collimation lens, BS is a beam splitter, P is a polarizer, SLM is a spatial light modulator, PM is a plane mirror
图 6不同轴向距离的实验结果图。(a)、 (d)分别为轴向偏移|Δz|=10 μm和|Δz|=15 μm时的涡旋相位波带片的相位分布图； (b)、 (c)分别是±10 μm处xy截面的光场强度分布；图 (e)、 (f)分别是±15 μm处xy截面的光场强度分布图
Figure 6.The experimental results with different axial shift distances. (a), (d) are the vortex phase distributions with |Δz|=10 μm and |Δz|=15 μm; (b), (c) are the total intensity distributions onxycross-section at 10 μm and −10 μm, respectively; (e), (f) are the total intensity distributions onxycross-section at 15 μm and −15 μm, respectively
图 7不同拓扑荷数xy截面光场分布实验图。图 (a)、 (b)、 (c)、 (d)分别为n=1、n=2、n=3和n=4时的波带片的相位分布图； (e)、 (f)、 (g)、 (h)分别为 (a)、 (b)、 (c)、 (d)对应波带片调制后的聚焦场在xy截面的光场分布
Figure 7.The experimental results of the focusing distribution onxycross-section with different topology charges. (a), (b), (c), (d) are the phase distributions of the zone plate withn=1,n=2,n=3 andn=4, respectively; (e), (f), (g), (h) are the corresponding experimental results for (a), (b), (c) and (d) after zone plate modulation, respectively
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