Light-Field Microscopy: a Review
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Modeling of Microlens Arrays with Different Lens Shapes Abstract
Modeling of Microlens Arrays with Different Lens Shapes Abstract Microlens arrays are found useful in many applications, such as imaging, wavefront sensing, light homogenizing, and so on. Due to different fabrication techniques / processes, the microlenses may appear in different shapes. In this example, microlens array with two typical lens shapes – square and round – are modeled. Because of the different apertures shapes, the focal spots are also different due to diffraction. The change of the focal spots distribution with respect to the imposed aberration in the input field is demonstrated. 2 www.LightTrans.com Modeling Task 1.24mm 4.356mm 150µm input field - wavelength 633nm How to calculate field on focal - diameter 1.5mm - uniform amplitude plane behind different types of - phase distributions microlens arrays, and how 1) no aberration does the spot distribution 2) spherical aberration ? 3) coma aberration change with the input field 4) trefoil aberration aberration? x z or x z y 3 Results x square microlens array wavefront error [휆] z round microlens array [mm] [mm] y y x [mm] x [mm] no aberration x [mm] (color saturation at 1/3 maximum) or diffraction due to square aperture diffraction due to round aperture 4 Results x square microlens array wavefront error [휆] z round microlens array [mm] [mm] y y x [mm] x [mm] spherical aberration x [mm] Fully physical-optics simulation of system containing microlens array or takes less than 10 seconds. 5 Results x square microlens array wavefront error [휆] z round microlens array [mm] [mm] y y x [mm] x [mm] coma aberration x [mm] Focal spots distribution changes with respect to the or aberration of the input field. -
Two-Photon Excitation Fluorescence Microscopy
P1: FhN/ftt P2: FhN July 10, 2000 11:18 Annual Reviews AR106-15 Annu. Rev. Biomed. Eng. 2000. 02:399–429 Copyright c 2000 by Annual Reviews. All rights reserved TWO-PHOTON EXCITATION FLUORESCENCE MICROSCOPY PeterT.C.So1,ChenY.Dong1, Barry R. Masters2, and Keith M. Berland3 1Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; e-mail: [email protected] 2Department of Ophthalmology, University of Bern, Bern, Switzerland 3Department of Physics, Emory University, Atlanta, Georgia 30322 Key Words multiphoton, fluorescence spectroscopy, single molecule, functional imaging, tissue imaging ■ Abstract Two-photon fluorescence microscopy is one of the most important re- cent inventions in biological imaging. This technology enables noninvasive study of biological specimens in three dimensions with submicrometer resolution. Two-photon excitation of fluorophores results from the simultaneous absorption of two photons. This excitation process has a number of unique advantages, such as reduced specimen photodamage and enhanced penetration depth. It also produces higher-contrast im- ages and is a novel method to trigger localized photochemical reactions. Two-photon microscopy continues to find an increasing number of applications in biology and medicine. CONTENTS INTRODUCTION ................................................ 400 HISTORICAL REVIEW OF TWO-PHOTON MICROSCOPY TECHNOLOGY ...401 BASIC PRINCIPLES OF TWO-PHOTON MICROSCOPY ..................402 Physical Basis for Two-Photon Excitation ............................ -
Multi-Perspective Stereoscopy from Light Fields
Multi-Perspective stereoscopy from light fields The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Changil Kim, Alexander Hornung, Simon Heinzle, Wojciech Matusik, and Markus Gross. 2011. Multi-perspective stereoscopy from light fields. ACM Trans. Graph. 30, 6, Article 190 (December 2011), 10 pages. As Published http://dx.doi.org/10.1145/2070781.2024224 Publisher Association for Computing Machinery (ACM) Version Author's final manuscript Citable link http://hdl.handle.net/1721.1/73503 Terms of Use Creative Commons Attribution-Noncommercial-Share Alike 3.0 Detailed Terms http://creativecommons.org/licenses/by-nc-sa/3.0/ Multi-Perspective Stereoscopy from Light Fields Changil Kim1,2 Alexander Hornung2 Simon Heinzle2 Wojciech Matusik2,3 Markus Gross1,2 1ETH Zurich 2Disney Research Zurich 3MIT CSAIL v u s c Disney Enterprises, Inc. Input Images 3D Light Field Multi-perspective Cuts Stereoscopic Output Figure 1: We propose a framework for flexible stereoscopic disparity manipulation and content post-production. Our method computes multi-perspective stereoscopic output images from a 3D light field that satisfy arbitrary prescribed disparity constraints. We achieve this by computing piecewise continuous cuts (shown in red) through the light field that enable per-pixel disparity control. In this particular example we employed gradient domain processing to emphasize the depth of the airplane while suppressing disparities in the rest of the scene. Abstract tions of autostereoscopic and multi-view autostereoscopic displays even glasses-free solutions become available to the consumer. This paper addresses stereoscopic view generation from a light field. We present a framework that allows for the generation However, the task of creating convincing yet perceptually pleasing of stereoscopic image pairs with per-pixel control over disparity, stereoscopic content remains difficult. -
Confocal Microscopy
Confocal microscopy Chapter in Handbook of Comprehensive Biophysics ( in press 2011) Elsevier Brad Amos MRC Laboratory of Molecular Biology, Hills Road, Cambridge CB2 0QH UK e-mail [email protected] Gail McConnell University of Strathclyde , Centre for Biophotonics 161 Cathedral Street , Glasgow G4 0RE UK [email protected] Tony Wilson Dept. of Engineering Science, University of Oxford, Parks Road, Oxford, OX1 3PJ, UK. eMail: [email protected] 1 Introduction A confocal microscope is one in which the illumination is confined to a small volume in the specimen, the detection is confined to the same volume and the image is built up by scanning this volume over the specimen, either by moving the beam of light over the specimen or by displacing the specimen relative to a stationary beam. The chief advantage of this type of microscope is that it gives a greatly enhanced discrimination of depth relative to conventional microscopes. Commercial systems appeared in the 1980s and, despite their high cost, the world market for them is probably between 500 and 1000 instruments per annum, mainly because of their use in biomedical research in conjunction with fluorescent labelling methods. There are many books and review articles on this subject ( e.g. Pawley ( 2006) , Matsumoto( 2002), Wilson (1990) ). The purpose of this chapter is to provide an introduction to optical and engineering aspects that may be o f interest to biomedical users of confocal microscopy. Flying-spot Microscopes A confocal microscope is a special type of ‘flying spot’ microscope. Flying spot systems were developed in the 1950s by combining conventional microscopes with electronics from TV and military equipment. -
Design and Fabrication of Flexible Naked-Eye 3D Display Film Element Based on Microstructure
micromachines Article Design and Fabrication of Flexible Naked-Eye 3D Display Film Element Based on Microstructure Axiu Cao , Li Xue, Yingfei Pang, Liwei Liu, Hui Pang, Lifang Shi * and Qiling Deng Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China; [email protected] (A.C.); [email protected] (L.X.); [email protected] (Y.P.); [email protected] (L.L.); [email protected] (H.P.); [email protected] (Q.D.) * Correspondence: [email protected]; Tel.: +86-028-8510-1178 Received: 19 November 2019; Accepted: 7 December 2019; Published: 9 December 2019 Abstract: The naked-eye three-dimensional (3D) display technology without wearing equipment is an inevitable future development trend. In this paper, the design and fabrication of a flexible naked-eye 3D display film element based on a microstructure have been proposed to achieve a high-resolution 3D display effect. The film element consists of two sets of key microstructures, namely, a microimage array (MIA) and microlens array (MLA). By establishing the basic structural model, the matching relationship between the two groups of microstructures has been studied. Based on 3D graphics software, a 3D object information acquisition model has been proposed to achieve a high-resolution MIA from different viewpoints, recording without crosstalk. In addition, lithography technology has been used to realize the fabrications of the MLA and MIA. Based on nanoimprint technology, a complete integration technology on a flexible film substrate has been formed. Finally, a flexible 3D display film element has been fabricated, which has a light weight and can be curled. -
Imaging with Second-Harmonic Generation Nanoparticles
1 Imaging with Second-Harmonic Generation Nanoparticles Thesis by Chia-Lung Hsieh In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2011 (Defended March 16, 2011) ii © 2011 Chia-Lung Hsieh All Rights Reserved iii Publications contained within this thesis: 1. C. L. Hsieh, R. Grange, Y. Pu, and D. Psaltis, "Three-dimensional harmonic holographic microcopy using nanoparticles as probes for cell imaging," Opt. Express 17, 2880–2891 (2009). 2. C. L. Hsieh, R. Grange, Y. Pu, and D. Psaltis, "Bioconjugation of barium titanate nanocrystals with immunoglobulin G antibody for second harmonic radiation imaging probes," Biomaterials 31, 2272–2277 (2010). 3. C. L. Hsieh, Y. Pu, R. Grange, and D. Psaltis, "Second harmonic generation from nanocrystals under linearly and circularly polarized excitations," Opt. Express 18, 11917–11932 (2010). 4. C. L. Hsieh, Y. Pu, R. Grange, and D. Psaltis, "Digital phase conjugation of second harmonic radiation emitted by nanoparticles in turbid media," Opt. Express 18, 12283–12290 (2010). 5. C. L. Hsieh, Y. Pu, R. Grange, G. Laporte, and D. Psaltis, "Imaging through turbid layers by scanning the phase conjugated second harmonic radiation from a nanoparticle," Opt. Express 18, 20723–20731 (2010). iv Acknowledgements During my five-year Ph.D. studies, I have thought a lot about science and life, but I have never thought of the moment of writing the acknowledgements of my thesis. At this moment, after finishing writing six chapters of my thesis, I realize the acknowledgment is probably one of the most difficult parts for me to complete. -
Super-Resolution Imaging by Dielectric Superlenses: Tio2 Metamaterial Superlens Versus Batio3 Superlens
hv photonics Article Super-Resolution Imaging by Dielectric Superlenses: TiO2 Metamaterial Superlens versus BaTiO3 Superlens Rakesh Dhama, Bing Yan, Cristiano Palego and Zengbo Wang * School of Computer Science and Electronic Engineering, Bangor University, Bangor LL57 1UT, UK; [email protected] (R.D.); [email protected] (B.Y.); [email protected] (C.P.) * Correspondence: [email protected] Abstract: All-dielectric superlens made from micro and nano particles has emerged as a simple yet effective solution to label-free, super-resolution imaging. High-index BaTiO3 Glass (BTG) mi- crospheres are among the most widely used dielectric superlenses today but could potentially be replaced by a new class of TiO2 metamaterial (meta-TiO2) superlens made of TiO2 nanoparticles. In this work, we designed and fabricated TiO2 metamaterial superlens in full-sphere shape for the first time, which resembles BTG microsphere in terms of the physical shape, size, and effective refractive index. Super-resolution imaging performances were compared using the same sample, lighting, and imaging settings. The results show that TiO2 meta-superlens performs consistently better over BTG superlens in terms of imaging contrast, clarity, field of view, and resolution, which was further supported by theoretical simulation. This opens new possibilities in developing more powerful, robust, and reliable super-resolution lens and imaging systems. Keywords: super-resolution imaging; dielectric superlens; label-free imaging; titanium dioxide Citation: Dhama, R.; Yan, B.; Palego, 1. Introduction C.; Wang, Z. Super-Resolution The optical microscope is the most common imaging tool known for its simple de- Imaging by Dielectric Superlenses: sign, low cost, and great flexibility. -
Microlens Array Grid Estimation, Light Field Decoding, and Calibration
1 Microlens array grid estimation, light field decoding, and calibration Maximilian Schambach and Fernando Puente Leon,´ Senior Member, IEEE Karlsruhe Institute of Technology, Institute of Industrial Information Technology Hertzstr. 16, 76187 Karlsruhe, Germany fschambach, [email protected] Abstract—We quantitatively investigate multiple algorithms lenslet images, while others perform calibration utilizing the for microlens array grid estimation for microlens array-based raw images directly [4]. In either case, this includes multiple light field cameras. Explicitly taking into account natural and non-trivial pre-processing steps, such as the detection of the mechanical vignetting effects, we propose a new method for microlens array grid estimation that outperforms the ones projected microlens (ML) centers and estimation of a regular previously discussed in the literature. To quantify the perfor- grid approximating the centers, alignment of the lenslet image mance of the algorithms, we propose an evaluation pipeline with the sensor, slicing the image into a light field and, in utilizing application-specific ray-traced white images with known the case of hexagonal MLAs, resampling the light field onto a microlens positions. Using a large dataset of synthesized white rectangular grid. These steps have a non-negligible impact on images, we thoroughly compare the performance of the different estimation algorithms. As an example, we apply our results to the quality of the decoded light field and camera calibration. the decoding and calibration of light fields taken with a Lytro Hence, a quantitative evaluation is necessary where possible. Illum camera. We observe that decoding as well as calibration Here, we will focus on the estimation of the MLA grid benefit from a more accurate, vignetting-aware grid estimation, parameters (to which we refer to as pre-calibration), which especially in peripheral subapertures of the light field. -
Development of Optical Hyperlens for Imaging Below the Diffraction Limit
Development of optical hyperlens for imaging below the diffraction limit Hyesog Lee, Zhaowei Liu, Yi Xiong, Cheng Sun and Xiang Zhang* 5130 Etcheverry Hall, NSF Nanoscale Science and Engineering Center (NSEC), University of California, Berkeley, CA 94720 *Corresponding author: [email protected] http://xlab.me.berkeley.edu Abstract: We report here the design, fabrication and characterization of optical hyperlens that can image sub-diffraction-limited objects in the far field. The hyperlens is based on an artificial anisotropic metamaterial with carefully designed hyperbolic dispersion. We successfully designed and fabricated such a metamaterial hyperlens composed of curved silver/alumina multilayers. Experimental results demonstrate far-field imaging with resolution down to 125nm at 365nm working wavelength which is below the diffraction limit. ©2007 Optical Society of America OCIS codes: (110 0180) Microscopy; (220.4241) Optical design and fabrication: Nanostructure fabrication References and links 1. E. Abbe, Arch. Mikroskop. Anat. 9, 413 (1873) 2. E. Betzig, J. K. Trautman, T. D. Harris, J. S. Weiner and R. L. Kostelak, “Breaking the diffraction barrier – optical microscopy on a nanometric scale,” Science 251, 1468-1470 (1991) 3. S. W. Hell, “Toward Fluorescence nanoscopy,” Nat. Biotechnol. 21, 1347-1355 (2003) 4. M. G. L. Gustafsson, “Nonlinear structured-illumination microscopy: Wide-field fluorescence imaging with theoretically unlimited resolution,” P. Natl. Acad. Sci. 102, 13081-13086 (2005) 5. J. B. Pendry, “Negative refraction makes a perfect lens,” Phys. Rev. Lett. 85, 3966-3969 (2000) 6. N. Fang, H. Lee, C. Sun and X. Zhang, “Sub-Diffraction-Limited Optical Imaging with a Silver Superlens” Science 308, 534-537 (2005) 7. -
Development of the Optical Microscope
White Paper Development of the Optical Microscope By Peter Banks Ph.D., Scientific Director, Applications Dept., BioTek Instruments, Inc. Products: Cytation 5 Cell Imaging Multi-Mode Reader An Optical Microscope commonly found in schools and universities all over the world. Table of Contents Ptolemy and Light Refraction --------------------------------------------------------------------------------------------- 2 Islamic Polymaths and Optics -------------------------------------------------------------------------------------------- 2 The First Microscope ------------------------------------------------------------------------------------------------------- 2 Hook and Micrographia --------------------------------------------------------------------------------------------------- 2 Van Leeuwenhoek and Animalcules ------------------------------------------------------------------------------------ 5 Abbe Limit -------------------------------------------------------------------------------------------------------------------- 6 Zernicke and Phase Contrast --------------------------------------------------------------------------------------------- 7 Fluorescence Microscopy ------------------------------------------------------------------------------------------------- 7 Confocal Microscopy ------------------------------------------------------------------------------------------------------- 8 BioTek Instruments, Inc. Digital Microscopy ---------------------------------------------------------------------------------------------------------- -
Scanning Confocal Microscopy with a Microlens Array
Scanning Confocal Microscopy with A Microlens Array Antony Orth*, and Kenneth Crozier y School of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA Corresponding authors: * [email protected], y [email protected] Abstract: Scanning confocal fluorescence microscopy is performed with a refractive microlens array. We simul- taneously obtain an array of 3000 20µm x 20µm images with a lateral resolution of 645nm and observe low power optical sectioning. OCIS codes: (180.0180) Microscopy; (180.1790) Confocal microscopy; (350.3950) Micro-optics High throughput fluorescence imaging of cells and tissues is an indispensable tool for biological research[1]. Even low-resolution imaging of fluorescently labelled cells can yield important information that is not resolvable in traditional flow cytometry[2]. Commercial systems typically raster scan a well plate under a microscope objective to generate a large field of view (FOV). In practice, the process of scanning and refocusing limits the speed of this approach to one FOV per second[3]. We demonstrate an imaging modality that has the potential to speed up fluorescent imaging over a large field of view, while taking advantage of the background rejection inherent in confocal imaging. Figure 1: a) Experimental setup. Inset: Microscope photograph of an 8x8 sub-section of the microlens array. Scale bar is 80µm. b) A subset of the 3000, 20µm x 20µm fields of view, each acquired by a separate microlens. Inset: Zoom-in of one field of view showing a pile of 2µm beads. The experimental geometry is shown in Figure 1. A collimated laser beam (5mW output power, λex =532nm) is focused into a focal spot array on the fluorescent sample by a refractive microlens array. -
Focus Cue Enabled Head-Mounted Display Via Microlens Array
Focus Cue Enabled Head-Mounted Display via Microlens Array Ryan Burke Leandra Brickson Stanford University Stanford University Electrical Engineering Department Electrical Engineering Department [email protected] [email protected] high field of view scene while still supporting focus cues. Abstract While these systems are good solutions for the A new head mounted display (HMD) is designed utilizing a vergence-accommodation conflict, they still are not as microlens array to resolve the vergence-accommodation accessible to the public as google cardboard. Our project conflict common in current HMDs. The hardware and investigates adding focus cues to the google cardboard software are examined via simulation to optimize a depth system via microlens array, eliminating the vergence and resolution tradeoff in this system to give the best -accommodation conflict. overall user experience. Ray tracing was used to design the optics so that all viewing zones were mapped to the eye to 2. Optical System Design provide focus cues. A program was also written to convert Lytro stereo pairs to a light field useable by the system. The proposed optical design of the focus cue enabled head mounted system is shown in figure 1. In this, the 1. Introduction google cardboard system is augmented by placing a microlens array (MLA) in front of the display to create a There has recently been a lot of research going into light field, which will then be projected to the virtual image developing consumer virtual reality (VR) systems aiming plane by the objective lens. In this system, the MLA will to give the user an immersive 3D experience through the create different viewing zones, which will provide depth use of head mounted displays.