* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download Precision High Numerical Aperture Scanning System for
Nonlinear optics wikipedia , lookup
Surface plasmon resonance microscopy wikipedia , lookup
Speed of light wikipedia , lookup
Nonimaging optics wikipedia , lookup
Retroreflector wikipedia , lookup
Scanning tunneling spectroscopy wikipedia , lookup
3D optical data storage wikipedia , lookup
Ultrafast laser spectroscopy wikipedia , lookup
Birefringence wikipedia , lookup
Photoconductive atomic force microscopy wikipedia , lookup
Scanning joule expansion microscopy wikipedia , lookup
Super-resolution microscopy wikipedia , lookup
Photonic laser thruster wikipedia , lookup
Vibrational analysis with scanning probe microscopy wikipedia , lookup
Optical aberration wikipedia , lookup
Photon scanning microscopy wikipedia , lookup
Anti-reflective coating wikipedia , lookup
Harold Hopkins (physicist) wikipedia , lookup
Optical coherence tomography wikipedia , lookup
Dispersion staining wikipedia , lookup
PRECISION HIGH NUMERICAL APERTURE SCANNING SYSTEM FOR FEMTOSECOND MICROMACHINING OF OCULAR MATERIALS OVER LARGE FIELD Daniel R. Brooks1, Nicolas S. Brown1, Lisen Xu1, Daniel E. Savage1, Wayne H. Knox1,2, Jonathan D. Ellis1,3 1 The Institute of Optics 2 Center for Visual Sciences 3 Department of Mechanical Engineering University of Rochester Rochester, New York In the past, the scanning of the focal region has been achieved by several different scanning methods. The first was a galvo-scanning system using two oscillating mirrors that are imaged into the entrance pupil of a high numerical aperture objective, thus changing the position of the focal spot. This method gives very good control and consistency but can only accomplish an approximately 300 μm scan range. In order to get a larger scan range, the scanning system was switched to two stacked piezo stepper stages with ±9 mm travel. In this mode, a sample is attached to the stages and is moved through the focal region, which is stationary. This method of scanning is not ideal because it requires the sample to move, which becomes impractical when writing structures in clinical applications. It was also found that the translation speed of these stages was inconsistent, varying up to 20 mm/s from a nominal speed of 100 mm/s. An example scan speed profile is shown in Figure. 1. 140 120 100 scan speed (mm/s) BACKGROUND Femtosecond laser micromachining has been developed for writing custom 3D refractive index modifications into ophthalmic hydrogels [1]. These results can be applied to the development of custom contact lenses, or customizing the refractive corrections in Intraocular lenses (IOLs). Recently, a design methodology has been demonstrated for writing lateral gradient index microlenses into hydrogels [2]. The writing process is due to accumulated thermal energy when a tightly focused laser beam experiences two-photon absorption in only the focal volume. This technology has now been demonstrated in writing refractive corrections directly into live cornea [3] where it is termed IRIS, for intratissue refractive surgery. Due to the nature of nonlinear absorption, the change in index only occurs in the focal region of the laser and is dependent on the speed the focal region is travelling through the material and power in the laser. In order to write efficiently, it is crucial to be able to reach scan speeds of up to 200 mm/s with reliable and consistent knowledge of the speed and position. The focal spot volume is on the order of 1 μm, thus high position accuracy is needed to ensure uniformity of the overlap and minimal scattering of the refractive structure. The scanning system must also be able to cover up to an 8 mm range to correct over the entire pupil of the eye. The requirements together put a high demand on the scanning stage and until now, a good solution that could accomplish both the accurate and consistent speed as well the required range has not been demonstrated. 80 60 40 20 0 7 7.05 7.1 time (s) 7.15 7.2 FIGURE 1. Scan speed profile of a piezo stepper stage with a displacement of 5 mm and a nominal speed of 100 mm/s. New scanning systems are needed to achieve the requirements of high speed, consistent scanning over a large range, when using exclusively high NA objectives. PROTYPE SCANNING SYSTEM To meet the previously stated requirements it became apparent that a new scanning system was needed. Previously a voice-coil type of scanner was developed for use in photoacoustic microscopy [4]. To achieve our goals we have developed a scanning solution in which an objective is attached to an oscillating flexure. The oscillator is attached to a z-axis stage which is in turn attached to a slower horizontal stage oriented perpendicular to the axis of the translation of the oscillator. First Version With the first version of this new stage, we were able to achieve consistent speeds and displacements with up to 2.5 mm of travel range. At higher ranges of motion, there was more variability of the end position which likely means that there was also more variability in the speed across the profile. This can be seen in Figures 2 and 3, which show two examples of structures written using this system in ophthalmic hydrogel polymers (used in contact lenses and intraocular lenses) Figure 2. Differential Interference Contrast Microscope photo of structure written at low speed (24 mm/s in middle, 9 Hz oscillation) in hydrogel. Edges are very consistent. Second Version Since the maximum range of the first version of our oscillating scan system was only approximately 2.5 mm, we are developing a second version of our oscillator scanning system with a custom flexure and driving motors. It should be able to achieve 8 mm of travel with consistent displacement and speed and a first resonance above 40 Hz. This will enable us to demonstrate writing of full field refractive structures over an 8 mm diameter area in under 5 minutes. We will demonstrate initial assessments of the refractive structures written in hydrogels and discuss the development of more sophisticated scanners for more advanced applications. FIGURE 3. Larger structure in hydrogel at higher speed (130 mm/s in middle, 9 Hz oscillation) shows more variability on edges. The total size of this structure is 2.31 mm in the direction of travel of the oscillator. REFERENCES [1] Ding L, Blackwell R, Kunzler J, Knox W. Large refractive index change in siliconebased and non-silicone-based hydrogel polymers induced by femtosecond laser micro-machining. Optics Express. 2006; 14: 11901-11909. [2] Xu L, Knox W. Lateral gradient index microlenses written in ophthalmic hydrogel polymers by femtosecond laser micromachining. Optical Materials Express. 2011; 1: 1416-1424 [3] Xu L, Knox W, DeMagistris M, Wang N, Huxlin K. Noninvasive Intratissue Refractive Index Shaping (IRIS) of the Cornea with Blue Femtosecond Laser Light. IOVS. 2011; 52: 8148-8155; published ahead of print September 19, 2011, doi:10.1167/iovs.11-7323. [4] Wang L, Maslov K, Yao J, Rao B, Wang L. Fast voice-coil scanning optical-resolution photoacoustic microscopy. OPTICS LETTERS. 2011; 36