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In recent years, vortex beams have become the focus of research, and their orbital angular momentum makes them have many important applications, like optical communication, particle manipulation, and optical measurement. At the same time, researchers are paying attention to more abundant generation methods. In previous studies, vortex beam generation methods are usually divided into two categories. The first category is the outcavity, such as spiral phase plate method, spatial light modulator method, mode conversion method, metasurface method, and corner array method, and the second category is the incavity, such as point-loss method, off-axis pumping method, and spatial light modulator method. However, these methods can not tolerate high power laser output and adjust topological charges flexibly. Therefore, how to generate a vortex beam that can tolerate high power laser output and adjust the topological charges flexibly is an important problem to be solved. Continuous surface deformation mirror is a key component of adaptive optical system. In the study of wavefront fitting for continuous surface deformation mirrors, there are usually two kinds of methods. The first type is model-free method, such as genetic algorithm, simulated annealing algorithm, stochastic parallel gradient descent (SPGD) algorithm, etc. These methods generally require many iterations and slow convergence, and it is difficult to change the topological charge flexibly. The second type is pattern method, such as Zernike mode method, Lukosz mode method, and enginmode method. This method first defines a set of complete orthogonal modes, calculates the mode coefficients, and completes the fitting of the target wavefront by linear superposition of each mode. Zernike mode is orthogonal in the circular domain, Lukosz mode is orthogonal in the circular domain derivative. However, usually the configuretion of deformation mirror is not circular domain. For example, the deformation mirror driver used in this paper is arranged in circular domain. In this case, the orthogonal basis needs to be rebuilt to use these two methods. The eigenmode of the deformed mirror is directly and precisely derived from the influence function of the deformed mirror drivers, so it can not only avoid the influence of fitting error, improve the fitting accuracy, but also adapt to the different configuration of the deformed mirror. Combined with the eigenmode method, continuous surface deformation mirror can fit all kinds of vortex beams with high precision and fast fitting speed, and can be applied to all kinds of deformation mirrors with different configurations. In this paper, the eigenmode method of continuous surface deformation mirror is used to simulate and analyze the fitting of the spiral wavefront of integer order with topological charge is −5 to 5, fractional order, multi-fractional order, and superposition state with the absolute value of topological charge less than 5. Various vortex light fields are generated by dynamic manipulation. The results show that the continuous surface deformation mirror will have a good application prospect in the field of high-power vortex field manipulation.
Schematic diagram of the vortex beam generated by continuous mirror deformation mirror
Schematic diagram of using DM to generate vortex beams.L1, L2, L3: convex lens; T: aperture; DM: deformation mirror; f: focal length
Fitting of the integer order spiral wavefront. (a)~(e) Target wavefront with the integer order l =1~5; (f)~(j) Fitting wavefront of the integer order l=1~5
Fitting of integer order vortex beams with topological charge is 2. (a) Unfiltered intensity at u2; (b) Filtered intensity at u4; (c) Unfiltered phase at u2; (d) Filtered phase at u4
The light field and phase of the integer order vortex beam after focusing and filtering. (a)~(d) Intensity with topological charges l=1, 3, 4, and 5; (e)~(h) Phase with topological charges l=1, 3, 4, and 5
Fitting of the fractional order spiral wavefront. (a)~(e) Target wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5; (f)~(j) Fitting wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5
Filtering results of the fractional order vortex beam. (a)~(e) Intensity of target wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5 at u4; (f)~(j) Intensity of fitting wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5 at u4
Filtering results of the fractional order vortex beam. (a)~(e) Phase of target wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5 at u4; (f)~(j) Phase of fitting wavefront with topological charges l=0.5, 1.5, 2.5, 3.5, and 4.5 at u4
Fitting of multi-fractional spiral wavefront. (a), (b) Target wavefront; (c), (d) Fitting wavefront
The light field and phase of the multi-fractional order target wavefront and the fitting wavefront after filtering. (a), (b) Intensity of multi-fractional order target wavefront at u4; (c), (d) Intensity of multi-fractional order fitting wavefront at u4; (e), (f) Phase of multi-fractional order target wavefront at u4; (g), (h) Phase of multi-fractional order fitting wavefront at u4
Superposition target wavefront and fitting wavefront. (a)~(d) Target wavefront with topological charges l=±1, ±2, ±3, and ±4; (e)~(h) Fitting wavefront with topological charges l=±1, ±2, ±3, and ±4
The light field and phase of the superposition fitting wavefront after filtering. (a)~(d) Intensity of fitting wavefront at with topological chrages l=±1,±2,±3, and ±4 at u4; (e)~(h) Phase of fitting wavefront at with topological chrages l=±1,±2,±3, and ±4 at u4
The mode purity of the superposition fitting wavefront after filtering. (a) l=±1; (b) l=±2; (c) l=±3; (d) l=±4
Dynamic manipulation of integer order vortex beams. (a1)~(a6) Intensity with topological charge l=2; (b1)~(b6) Spiral phase with topological charge l= 2; (c1)~(c6) Intensity with topological charge l=3; (d1)~(d6) Spiral phase with topological charge l= 3