光学学报, 2019, 39 (1): 0126001, 网络出版: 2019-05-10
新型矢量光场调控:简介、进展与应用 
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Manipulation on Novel Vector Optical Fields: Introduction, Advances and Applications
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图 1. (a)庞加莱球及(b)球上的偏振态分布[30]
Fig. 1. (a) Poincare sphere and (b) the distribution of polarization on the sphere[30]
图 2. 杂化偏振矢量光场与径向偏振矢量光场的对比[30]。(a)杂化偏振矢量光场;(b)径向偏振矢量光场
Fig. 2. Comparison of hybridly polarized and radially polarized vector optical fields[30]. (a) Hybridly polarized vector optical field; (b) radially polarized vector optical field
图 3. 杂化偏振矢量光场和径向偏振矢量光场的强度分布[30]
Fig. 3. Intensity distribution of hybridly polarized vector optical field and radially polarized vector optical field[30]
图 4. 利用光轴取向为45°和0°的1/4波片得到的旋向变化杂化偏振矢量光场[31]。(a)(b)偏振态分布;(c)(d)强度分布
Fig. 4. Distributions of (a)(b) polarization and (c)(d) intensity pattern of the azimuthally varying hybridly polarized vector optical fields with 45° and 0° quarter wave plate, respectively[31]
图 5. 旋向变化的杂化偏振矢量光场成丝的数值模拟[55]
Fig. 5. Simulated collapsing patterns of the azimuthally varying hybridly polarized vector optical fields[55]
图 6. 椭偏率空间变化的矢量光场的强度和偏振态分布[56]
Fig. 6. Distribution of intensity and polarization of ellipticity-variant vector optical fields[56]
图 7. 径向变化的杂化偏振矢量光场的偏振态分布示意图、强度和斯托克斯参量实验结果[70]
Fig. 7. Simulated distribution of polarization, measured intensity patterns and Stokes parameters of radially variant vector optical field with hybrid state of polarization[70]
图 8. 径向变化的杂化偏振矢量光场聚焦后被用于驱动微粒运动[70]
Fig. 8. Snapshots of the motion of trapped particles around the ring focus generated by radially variant vector optical fields with hybrid state of polarization[70]
图 11. 全庞加莱球矢量光场产生二次谐波[77]。(a)基频全庞加莱球矢量光场的强度和偏振态分布;(b)二次谐波理论强度分布;(c)实验产生的二次谐波的强度分布
Fig. 11. Second harmonic generation with full Poincare sphere beams[77]. (a) Intensity and polarization distributions of fundamental full Poincare sphere beams; (b) numerical simulations of the intensity patterns of the second harmonic light field; (c) experimental results for the intensity patterns of the second harmonic light field
图 12. 拓扑荷为±1的高阶庞加莱球[34]
Fig. 12. Higher-order Poincare sphere representation for the ±1 topological charges[34]
图 13. 高阶庞加莱球上矢量光场的偏振态和强度分布[80]
Fig. 13. Polarization and intensity distributions of the vector optical fields on the higher-order Poincare sphere[80]
图 14. 杂化阶庞加莱球[35]。(a)~(c)点A、B、C处光场的相位分布;(d)~(f)对应的强度和偏振态分布
Fig. 14. Hybrid-order Poincare sphere[35]. (a)-(c) Phases for optical fields at points A, B, and C, respectively; (d)-(f) corresponding intensity and polarization distributions
图 16. 携带OAM的广义庞加莱球上的矢量光场[84]
Fig. 16. Vector optical fields on generalized Poincare sphere carrying OAM[84]
图 17. 包含7个矢量光场“基元”的阵列矢量光场及其弱聚焦情况[37]。(a)(b)径向场和旋向场作为“基元”构成的阵列矢量光场;(c)~(e)阵列矢量光场的“基元”、“点阵”和总场的弱聚焦场;(f)弱聚焦场在硅表面烧蚀的SEM图像
Fig. 17. Array vector optical fields with seven vector optical field bases and the weakly focused status[37]. (a)(b) Array vector optical fields with radially and azimuthally polarized vector optical fields as bases, respectively; (c)-(e) weakly focused fields of the base, lattice, and array vector optical field; (f) SEM image of the silicon surface ablated by the weakly focused fields
图 18. 由旋向矢量光场“基元”构成的阵列矢量光场和利用其紧聚焦场进行微加工的SEM图像[38]。(a)~(e)阵列矢量光场的总强度;(f)~(j)阵列矢量光场的x分量强度;(k)~(o)阵列矢量光场的紧聚焦场在硅表面烧蚀的SEM图像
Fig. 18. Array vector optical fields with azimuthally polarized vector optical fields as bases and SEM images of micromachined silicon with the tightly focused fields[38]. (a)-(e) Total intensity patterns of the array vector optical fields; (f)-(j) x-component intensity patterns of the array vector optical fields; (k)-(o) SEM images of the silicon surfaces ablated by the tightly focused array vector optical fields
图 19. 具有空间变化参数的分形光场[39]。(a)振幅;(b)相位;(c)偏振;(d)振幅-相位;(e)相位-偏振;(f)振幅-偏振;(g)振幅-相位-偏振
Fig. 19. Fractal optical fields with the space-variant parameters[39]. (a) Amplitude-only; (b) phase-only; (c) polarization-only; (d) amplitude-phase; (e) phase-polarization; (f) amplitude-polarization; (g) amplitude-phase-polarization
图 20. 基于谢尔宾斯基地毯构造的两类典型分形矢量光场的偏振态和强度分布[39]。(a)(b)偏振态分布;(c)(d)总光强实验结果;(e)(f) x分量强度实验结果
Fig. 20. Polarization and intensity distributions of two types of fractal vector optical fields based on the Sierpinski structure[39]. (a)(b) Polarization states; (c)(d) experimental total intensity patterns; (e)(f) experimental x-component intensity patterns
图 21. 以径向偏振矢量光场为“基元”并与不同分形“点阵”结合的分形矢量光场的强度实验结果[40]
Fig. 21. Experimental intensity patterns of the generated fractal vector optical fields with radially polarized vector optical fields as bases and different lattices[40]
图 22. B类分形矢量光场在焦面上产生的阵列矢量光场[39]。(a)焦场强度模拟结果,图片尺寸0.6 mm×0.6 mm;(b)焦场强度模拟结果,图片尺寸1.8 mm×1.8 mm;(c)焦场强度模拟结果,图片尺寸5.4 mm×5.4 mm;(d)焦场强度实验结果
Fig. 22. Array vector fields at the focal planes of the type-B fractal vector optical fields[39]. (a) Simulation results of focused field intensity for dimension of 0.6 mm×0.6 mm; (b) simulation results of focused field intensity for dimension of 1.8 mm×1.8 mm; (c) simulation results of focused field intensity for dimension of 5.4 mm×5.4 mm; (d) experimental results of focused field intensity
图 23. 多区域扇形掩模板和阵列矢量焦场[86-87]。(a)沿径向分割的多区域扇形掩模板;(b)沿旋向分割的多区域扇形掩模板;(c)图(a)对应生成的阵列矢量焦场;(d)图(b)对应生成的阵列矢量焦场
Fig. 23. Multi-zone sector plates and corresponding array vectorial focused fields[86-87]. (a) Multi-zone plate divided in radial direction; (b) multi-zone plate divided in azimuthal direction; (c) vectorial focused fields corresponding to (a); (d) vectorial focused fields corresponding to (b)
图 24. 二维矢量焦点阵列[88]。(a)焦点强度和位置可调;(b)焦点偏振态可调
Fig. 24. Two-dimensional vectorial multifocal array[88]. (a) Multifocal spots with controllable intensities and positions; (b) multifocal spots with controllable states of polarization
图 25. 焦点参数可控的三维矢量焦点阵列[88]。(a)三维矢量焦点阵列;(b)~(e)经过偏振片之后的强度,红色箭头为偏振片的透射方向
Fig. 25. Three-dimensional vectorial multifocal array with controllable parameters[88]. (a) Three-dimensional vectorial multifocal array; (b)-(e) corresponding intensity patterns of beams passing a polarizer with transmission direction marked by a red double arrow
图 26. 阵列矢量光场的动态调控及应用。(a)旋转阵列矢量光场和相应的焦场轨迹模拟图[89];(b)剪切变换阵列分形矢量光场和相应的微操纵实验图[40]
Fig. 26. Dynamically controlled array vector optical fields and the applications. (a) Rotation of the array vector optical field and the corresponding simulated focal traces[89]; (b) shear transformation of the array fractal vector optical field and the corresponding trapping experiment results[40]
图 27. 两种全庞加莱球场以及其中的C点和L线
Fig. 27. Two kinds of full Poincare beams and C-point and L-line in these fields
图 28. 出射场的强度和偏振态分布(偏振C点用圆圈表示,L线用黄色线圈表示)[93]
Fig. 28. Intensity and polarization distributions of the output field (the C-points are marked by circles, and the L-line is represented by a yellow line)[93]
图 29. 具有不同振幅比的三光束干涉生成的偏振奇点阵列矢量光场(绿色椭圆代表偏振态,黄色曲线代表L线,蓝色圆环和红色方块代表C点)[41]。(a) 1∶1∶1;(b) 5∶5∶7;(c) 5∶5∶3
Fig. 29. Arrayed polarization singularity vector optical fields generated by interference of three polarized waves with different amplitude ratios (the green ellipses show the polarization states, the yellow lines indicate L-lines, and the blue circles and red squares represent the C-points)[41]. (a) 1∶1∶1; (b) 5∶5∶7; (c) 5∶5∶3
图 30. 类电场线形式的多偏振奇点矢量光场[42]
Fig. 30. Multiple polarization singularity vector optical fields with spatial state of polarization (SoP) structures similar to the electric field lines[42]
图 31. 六种多奇点矢量光场的偏振分布[43]
Fig. 31. Polarization distributions of six kinds of multiple polarization singularity vector optical fields[43]
图 32. 二维正交坐标系。(a)抛物坐标系;(b)椭圆坐标系;(c)双极坐标系;(d)双曲坐标系
Fig. 32. Two-dimensional orthogonal coordinates systems. (a) Parabolic coordinates system; (b) elliptic coordinates system; (c) bipolar coordinates system; (d) hyperbolic coordinates system
图 33. n=0时不同拓扑荷情况下的抛物对称矢量光场[44]
Fig. 33. Parabolic-symmetry vector optical fields with different topological charges and n=0[44]
图 34. n=0时不同拓扑荷情况下的椭圆对称矢量光场[45]
Fig. 34. Elliptic-symmetry vector optical fields with different topological charges and n=0[45]
图 35. n=0时不同拓扑荷情况下的双极对称矢量光场[46]
Fig. 35. Bipolar-symmetry vector optical fields with different topological charges and n=0[46]
图 36. n=0时不同拓扑荷情况下的双曲对称矢量光场[47]
Fig. 36. Hyperbolic-symmetry vector optical fields with different topological charges and n=0[47]
图 37. 具有阿基米德螺旋线形式偏振态分布的焦场[48]
Fig. 37. Polarization structure in the focal plane depicted by Archimedean spiral pattern[48]
图 38. 任意焦场调控[49]。(a)庞加莱球;(b)~(b3)焦场斯托克斯参量的理论模拟;(c)~(c3)相应的实验结果
Fig. 38. Arbitrarily designed focal fields[49]. (a) Poincare sphere; (b)-(b3) simulated Stokes parameters of the vectorial focal field; (c)-(c3) corresponding experimental results
图 39. 偏振态随轨迹线变化的三维矢量焦场:焦平面上的二维圆环和三维空间分布的阿基米德螺旋线三维矢量[105]
Fig. 39. Experimentally generated vectorial focal fields consisting of 2D ring curve and 3D Achimedean curve with continuously varying state of polariza-tion. The 2D ring is located at the focal plane[105]
图 40. 两种椭圆对称的矢量光场[51]。(a)椭圆径向对称;(b)椭圆旋向对称
Fig. 40. Two vector optical fields with elliptical symmetry[51]. (a) With elliptical radial symmetry; (b) with elliptical azimuthal symmetry
图 41. 太极图案矢量光场[106]。(a)总强度分布;(b)x分量强度分布;(c)y分量强度分布;(d)偏振态分布
Fig. 41. Vector optical field with Taiji pattern[106]. (a) Total intensity pattern; (b) x-component intensity pattern; (c) y-component intensity pattern; (d) state of polarization distribution
图 42. 联合调控光场的振幅、偏振态和相位[107]。入射矢量光场的(a)强度、(b)偏振态和(c)相位示意图;(d)总强度均匀分布的三角形焦斑
Fig. 42. Comprehensive adjustment of optical field amplitude, state of polarization, and phase[107]. (a) Total intensity, (b) state of polarization, and (c) phase of the incident vector optical field; (d) triangle focal spot with uniform intensity
潘岳, 丁剑平, 王慧田. 新型矢量光场调控:简介、进展与应用[J]. 光学学报, 2019, 39(1): 0126001. Yue Pan, Jianping Ding, Huitian Wang. Manipulation on Novel Vector Optical Fields: Introduction, Advances and Applications[J]. Acta Optica Sinica, 2019, 39(1): 0126001.
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