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Deformable mirror (DM) represent the most convenient tool forwavefront control and correction of optical aberrations. Deformable mirrors are used in combination with wavefront sensors and real-time control system in adaptive optics. They are also finding a new use in femtosecond pulse shaping *. The shape of the DM can be controlled with a speed that is appropriate for compensation of dynamic aberrations present in the optical system. In practice the DM shape should be changed much faster than the process that should be corrected, as the correction process, even for a static aberration, may take several iterations. A DM usually has many degrees of freedom. Typically, these degrees of freedom are associated with the mechanical actuators and it can be roughly taken that one actuator corresponds to one degree of freedom.
Deformable mirror parameters Number of actuators determines the number of degrees of freedom (wavefront inflections) the mirror can correct. It is very common to compare an arbitrary DM to an ideal device that can perfectly reproduce wavefront modes in the form of Zernike polynomials. For predefined statistics of aberrations a deformable mirror with M actuators can be equivalent to an ideal Zernike corrector with N (usually N < M) degrees of freedom. For correction of the atmospheric turbulence, elimination of low-order Zernike terms usually results in significant improvement of the image quality, while further correction of the higher-order terms introduces less significant improvements. For strong and rapid wavefront error fluctuations such as shocks and wake turbulence typically encountered in high-speed aerodynamic flowfields, the number of actuators, actuator pitch and stroke determine the maximum wavefront gradients that can be compensated for. Actuator pitch is the distance between actuator centers. Deformable mirrors with large actuator pitch and large number of actuators are bulky and expensive. Actuator stroke is the maximum possible actuator displacement, typically in positive or negative excursions from some central null position. Stroke typically ranges from ±1 to ±10 microns. Free actuator stroke limits the maximum amplitude of the corrected wavefront, while the inter-actuator stroke limits the maximum amplitude and gradients of correctable higher-order aberrations. Influence function is the characteristic shape corresponding to the mirror response to the action of a single actuator. Different types of deformable mirrors have different influence functions, moreover the influence functions can be different for different actuators of the same mirror. Influence function that covers the whole mirror surface is called a "modal" function, while localized response is called "zonal". Actuator coupling shows how much the movement of one actuator will displace its neighbors. All "modal" mirrors have large cross-coupling, which in fact is good as it secures the high quality of correction of smooth low-order optical aberrations that usually have the highest statistical weight. Response time shows how quickly the mirror will react to the control signal. Can vary from microseconds (MEMS mirrors) to tens of seconds for thermally controlled DM's. Hysteresis and creep are nonlinear actuation effects that decrease the precision of the response of the deformable mirror. For different concepts, the hysteresis can vary from practically zero (membrane mirrors) to tens of percent for mirrors with piezoelectric actuators. Hysteresis is a residual positional error from previous actuator position commands, and limits the mirror ability to work in a feedforward mode, outside of a feedback loop. Deformable mirror concepts Segmented deformable mirrors are formed by independent flat mirror segments. Each segment can move a small distance back and forward to approximate the average value of the wavefront over the patch area. Normally these mirror have little or zero cross-talk between actuators. Stepwise approximation works bad for smooth continuous wavefronts. Sharp edges of the segments and gaps between the segments contribute to the light scattering, limiting the applications to those non-sensitive to scattered light. Considerable improvement of the approximation performance of the segmented mirror can be achieved by introduction of three degrees of freedom per segment: piston tip and tilt. These mirrors require three times more actuators than piston segmented mirrors and they suffer from diffraction on the segment edges. This concept was used for fabrication of large segmented primary mirrors of Keck telescopes. Continuous faceplate deformable mirrors with discrete actuators are formed by the front surface of a thin deformable plate. The shape of the plate is controlled by a number of discrete actuators that are fixed to its back side. The shape of the mirror depends on the combination of forces applied to the faceplate, boundary conditions (the way the plate is fixed to the mirror) and the geometry and the material of the plate. These mirrors considered to be the best, as they allow smooth wavefront control with very large - up to several thousands - degrees of freedom. Membrane deformable mirror are formed by a thin conductive and reflective membrane stretched over a solid flat frame. The membrane can be deformed electrostatically by applying control voltages to the electrostatic electrode actuators that can be positioned under the membrane and also over the membrane. If there are any electrodes positioned over the membrane, they should be transparent. It is possible to operate the mirror with only one group of electrodes positioned under the mirror. In this case a bias voltage should be applied to all electrodes, to make the membrane initially spherical. The membrane can move back and forth with respect to the reference sphere. MEMS deformable mirrors are fabricated using technologies or bulk or surface micromachining. MEMS mirrors have a great potential to be cheap. They can break the high price threshold of the conventional adaptive optics. Bimorph deformable mirrors are formed by two or more layers of different materials. One or more of (active) layers are fabricated from a piezoelectric or electrostrictive material. Electrode structure is patterned on the active layer to facilitate local response. The mirror is deformed when a voltage is applied to one or more of its electrodes, causing them to extend laterally, which results in local mirror curvature. Bimorph mirrors are rarely made with more than 100 electrodes. 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