2) Basic Physical Optics-Pedrotti
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PHYSICS 4420 Physical Optics Fall 2017 Lecture Section 001, Physics Room 311, MWF 11:00–11:50 A.M
PHYSICS 4420 Physical Optics Fall 2017 Lecture Section 001, Physics Room 311, MWF 11:00–11:50 a.m. Recitation Sections 201, Physics Room 311, W 1–1:50 p.m. Professor: Bibhudutta Rout Rout’s Office: Physics Bldg., Room 007 Telephone: (940) 369-8127 E-mail: [email protected] Office Hours: M 9:30a.m.–10:30 a.m., and by appointment Prerequisite: PHYS 2220 Text: Principles of Physical Optics, by C.A. Bennett, Wiley 2008, ISBN 10 0-470-12212-9. A useful reference is Optics, 4th Edition, by Eugene Hecht, Pearson 2002, ISBN 0-8053-8566-5. Exams: There will be two in-class exams during the semester, and a comprehensive final exam. Exam questions will be based on material covered in the lecture, contained in the text, and in the homework assignments. There will be no makeup exams. Homework: Homework sets will be assigned and collected each week. You may collaborate on the homework, but the solutions you hand in must represent your own intellectual effort. You must present complete explanations to receive full credit. Participation: Part of your grade will be based on your participation in recitation, in which problem solutions will be discussed and students will be expected to contribute. You will also be required to give a 10 minute talk in recitation on an approved topic of interest to you related to optics and not covered in class. Grade: The grading in the course will be based on the total points earned from exams and homework as follows: Exams 20 points for each of the two in-class exams 30 points for the final Homework 20 points Participation/Attendance 10 points Total 100 points Note: This document is for informational purposes only and is subject to change upon notification. -
Mono and Multifocals.Wps
Monovision and Multifocal Lenses THE GOAL: To provide you good functional vision without glasses at both distance and near most of the time. There are some demanding visual tasks in which monovision or multifocal (bifocal) lenses may not provide acceptable vision and additional glasses may be needed. MONOVISION Monovision interrupts the natural binocular (both eyes together) vision process by using one eye for distance viewing (usually the dominant eye) and the other eye for intermediate and near viewing. This is not how our visual systems were made, but monovision is an accepted modality and has been used for decades. Adapting to having one eye for distance and one for near takes time to adjust to , and is something that is very easy for some and very difficult for others. As the adaptation process proceeds vision becomes clear at all distances, as the brain suppresses the eye that is not being used. Initially you may feel that your distance vision is blurred by your near eye, as your near eye is focused for near and intermediate distances. This perception of distance blur should be reduced over time as the brain learns to suppress the near eye. Noticing a reduction in stereo vision, or depth perception is normal , as the eyes are not working, or teamed together. Noticing a mild reduction in night vision is normal with monovision. Everybody adapts differently , but is good to continue to try monovision for several consecutive days, or longer, to let the adaptation process begin. Monovision is a learned technique, and everybody’s timetable for adaptation is different. -
Scattering Characteristics of Simplified Cylindrical Invisibility Cloaks
Scattering characteristics of simplified cylindrical invisibility cloaks Min Yan, Zhichao Ruan, Min Qiu Department of Microelectronics and Applied Physics, Royal Institute of Technology, Electrum 229, 16440 Kista, Sweden [email protected] (M.Q.) Abstract: The previously reported simplified cylindrical linear cloak is improved so that the cloak’s outer surface is impedance-matched to free space. The scattering characteristics of the improved linear cloak is compared to the previous counterpart as well as the recently proposed simplified quadratic cloak derived from quadratic coordinate transforma- tion. Significant improvement in invisibility performance is noticed for the improved linear cloak with respect to the previously proposed linear one. The improved linear cloak and the simplified quadratic cloak have comparable invisibility performances, except that the latter however has to fulfill a minimum shell thickness requirement (i.e. outer radius must be larger than twice of inner radius). When a thin cloak shell is desired, the improved linear cloak is much more superior than the other two versions of simplified cloaks. ©2007 OpticalSocietyofAmerica OCIS codes: (290.5839) Scattering, invisibility; (260.0260) Physical optics; (999.9999) Invis- ibility cloak. References and links 1. J. B. Pendry, D. Schurig, and D. R. Smith, “Controlling electromagnetic fields,” Science 312, 1780–1782 (2006). 2. U. Leonhardt, “Optical conformal mapping,” Science 312, 1777–1780 (2006). 3. A. Al`u, and N. Engheta, “Achieving transparency with plasmonic and metamaterial coatings,” Phys. Rev. E 72, 016,623 (2005). 4. Z. Ruan, M. Yan, C. W. Neff, and M. Qiu, “Ideal cylindrical cloak: Perfect but sensitive to tiny perturbations,” Phys. Rev. Lett. 99, 113,903 (2007). -
Descartes' Optics
Descartes’ Optics Jeffrey K. McDonough Descartes’ work on optics spanned his entire career and represents a fascinating area of inquiry. His interest in the study of light is already on display in an intriguing study of refraction from his early notebook, known as the Cogitationes privatae, dating from 1619 to 1621 (AT X 242-3). Optics figures centrally in Descartes’ The World, or Treatise on Light, written between 1629 and 1633, as well as, of course, in his Dioptrics published in 1637. It also, however, plays important roles in the three essays published together with the Dioptrics, namely, the Discourse on Method, the Geometry, and the Meteorology, and many of Descartes’ conclusions concerning light from these earlier works persist with little substantive modification into the Principles of Philosophy published in 1644. In what follows, we will look in a brief and general way at Descartes’ understanding of light, his derivations of the two central laws of geometrical optics, and a sampling of the optical phenomena he sought to explain. We will conclude by noting a few of the many ways in which Descartes’ efforts in optics prompted – both through agreement and dissent – further developments in the history of optics. Descartes was a famously systematic philosopher and his thinking about optics is deeply enmeshed with his more general mechanistic physics and cosmology. In the sixth chapter of The Treatise on Light, he asks his readers to imagine a new world “very easy to know, but nevertheless similar to ours” consisting of an indefinite space filled everywhere with “real, perfectly solid” matter, divisible “into as many parts and shapes as we can imagine” (AT XI ix; G 21, fn 40) (AT XI 33-34; G 22-23). -
CHAPTER 1 PHYSICAL OPTICS: INTERFERENCE • Introduction
CHAPTER 1 PHYSICAL OPTICS: INTERFERENCE What is “physical optics”? • Introduction The methods of physical optics are used when the • Waves wavelength of light and dimensions of the system are of • Principle of superposition a comparable order of magnitude, when the simple ray • Wave packets approximation of geometric optics is not valid. So, it is • Phasors • Interference intermediate between geometric optics, which ignores • Reflection of waves wave effects, and full wave electromagnetism, which is a precise theory. • Young’s double-slit experiment • Interference in thin films and air gaps In General Physics II you studied some aspects of geometrical optics. Geometrical optics rests on the assumption that light propagates along straight lines and is reflected and refracted according to definite laws, such Or the use of a convex lens as a magnifying lens: as Fermat’s principle and Snell’s Law. As a result the positions of images in mirrors and through lenses, etc. can be determined by scaled drawings. For example, the s ! s production of an image in a concave mirror. s Object object y Image • F • C f f y ! image 2 s ! 1 But many optical phenomena cannot be adequately The colors you see in a soap bubble are also due to an explained by geometrical optics. For example, the interference effect between light rays reflected from the iridescence that makes the colors of a hummingbird so front and back surfaces of the thin film of soap making brilliant are not due to pigment but to an interference the bubble. The color depends on the thickness of film, effect caused by structures in the feathers. -
Suzi Fleiszig Researches the Cornea's Resistance To
UNIVERSITY OF CALIFORNIA VOL. 2, NO. 1 | FALL 2009 Berkeley Optometry magazine SUZI FLEISZIG RESEARCHES THE CORNEA’S RESISTANCE TO INFECTION ADVANCING EDUCATION AND RESEARCH AT BERKELEY OPTOMETRY EXECUTIVE EDITOR Lawrence Thal dean’s message MANAGING EDITOR Jennifer C. Martin EDITOR Barbara Gordon EXECUTIVE ART DIRECTOR Molly Sharp E ARE BLESSED TO LIVE IN “INTERESTING TIMES”! PHOTOGRAPHY WAt this writing, the U.S. economy is in the tank, the state of California Ken Huie is in the red, and I’m sure I don’t need to tell you that the budget situation at the University of California continues to be challenging. PRODUCTION MANAGER Molly Sharp In this environment, our priorities are to preserve and maintain our funda- mental missions—teaching, research, and public service. And I’m pleased to say WRITERS/CONTRIBUTORS that Berkeley Optometry continues to excel in all of these through the efforts of Suzi Fleiszig, Lu Chen, Cynthia Dizikes, our dedicated faculty and staff. In this spirit, it seems timely to celebrate some Lawrence Thal, Mika Moy, Pam of the highlights of the last year. Satjawatcharaphong, Joy Sarver Among other things, in this issue of Berkeley Optometry Magazine you will see DESIGN that we have a new faculty and student exchange agreement with Peking Medi- ContentWorks, Inc. cal University (PKU) Third Hospital; one of our students, Brian Snydsman, won the 2008 Essilor Optometry Superbowl at the annual meeting of the American Optometric Association and American Optometric Student Asso- Published by University of California, Berkeley, ciation; Professor Clifton Schor received the Charles F. Prentice Medal from School of Optometry Office of External the American Academy of Optometry at its annual meeting last October; and Relations and Professional Affairs Professor Suzanne Fleiszig (see cover) and David Evans won a grant from the Phone: 510-642-2622, Fax: 510-643-6583 Bill and Melinda Gates Foundation as part of the global Grand Challenges Send comments and letters to: Explorations initiative. -
Corneal Haze and Visual Outcome After Collagen Crosslinking for Keratoconus: a Comparison Between Total Epithelium Off and Partial Epithelial Removal Methods
Original Article Corneal haze and visual outcome after collagen crosslinking for keratoconus: A comparison between total epithelium off and partial epithelial removal methods Hasan Razmjoo, Behrooz Rahimi, Mona Kharraji1, Nima Koosha, Alireza Peyman Department of Ophthalmology, 1Medical Student Research Committee, Isfahan University of Medical Sciences, Isfahan, Iran Abstract Background: Keratoconus is an asymmetric, bilateral, progressive noninflammatory ectasia of the cornea that affects approximately 1 in 2000 of the general population. This may cause a significant negative impact on quality of life. Corneal collagen crosslinking (CXL) is one of the recently introduced methods that have been used to decrease the progression of keratoconus, in particular, as well as other corneal‑thinning processes. Materials and Methods: A total of 44 keratoconic eyes of 22 patients were enrolled in this randomized prospective study, after obtaining informed consent. In the first group, the corneal epithelium were totally removed and in the second group, the central 3 mm of epithelium was kept intact and partial removal was performed. After collagen crosslinking in both groups, comprehensive ophthalmologic examination was performed on all patients before and 6 months after the surgery. This article is registered at www.clinicaltrial.gov with registration number NCT01809977. Results: The difference between the two groups was not statistically significant regarding postoperative corneal haziness, refraction, and visual acuity (P > 0.05). However, comparison of pre‑ and postoperative parameters within each group revealed that total removal of the cornea has resulted in significant improvement of K‑max (P value: 0.01) and Q‑value (P value: 0.009); while eyes in partial removal group had better improvement of corrected vision (P value: 0.006). -
Light Propagation Through the Eye: Numerical Considerations and Applications to Presbylasik Surgery Analysis
Light propagation through the eye: numerical considerations and applications to presbylasik surgery analysis Julián Espinosa Tomás Optics Department, University of Alicante Group of Optics and Vision Science Carlos Illueca, PhD. David Mas, PhD. Jorge Pérez, PhD. Julián Espinosa, MSc. Vissum Corporation, Alicante Jorge Alió, PhD. Dolores Ortiz, PhD. Esperanza Sala, OD. Light patterns calculation inside the eye Transmittance evaluation of cornea Transmittance evaluation of crystalline lens Wave propagation (angular spectrum) up to the plane of interest. Applications to presbylasik surgery analysis Corneal transmittance evaluation: - Geometrical configuration 2 surfaces 1st surface: Corneal topography 2nd surface: Dubbelman 2003 =6.6 − 0.005 × 2 2 2 R2 age xy+ +(1 + Qz2 ) − 2 Rz 2 = 0 Q2 = −0.1 − 0.007 × age Corneal transmittance evaluation: - Optical path length Crystalline lens transmittance evaluation Dubbelman 2001 (Scheimpflug photography ) x2+ y 2 +(1 + Qz ) 2 − 2 Rz = 0 = − × =−6.4 + 0.03 × Rant 12.9 0.057 age ; Qant age =− + × =−6.0 + 0.07 × Rpost 6.2 0.012 age ; Qpost age Crystalline lens transmittance evaluation opznzzii≈+1( 21 ii −)cosδ 102 i +∆−( z i) cos ( δ 12 ii + δ ) Wave propagation Convergent patterns calculation λz exp −iπ m ɶ 2 × ()∆x 2 0 ()u∝ DFT −1 z µ 2 m∆ x m2 ()∆ x ×DFT u0 − i π 0 1 0 exp 2 N λ N z c ∆x2 z≤0 ≤ z Nyquist condition λN c zc = 20mm λ = 633nm Total eye ∆x= 6.7mm N = 3600 0 Φ =3 ∆x p()4 0 Wave propagation 2 ∆x0 Nyquist condition: Nλ ≥ zc N κ >1 N′ = λ′ = κλ Let us define , κ and 1 1 ∆ξ ∆ξ = ∆ξ ′ = = ′ δ x0 δx0 κ ′ ′ ∆x0 ∆ξ = N ∆x0 = ∆ x z ∆ξ′ ∆x= N ′ z Wave propagation Rectangle function κ=1 vs. -
A Novel Vertebrate Eye Using Both Refractive and Reflective
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Current Biology 19, 108–114, January 27, 2009 ª2009 Elsevier Ltd All rights reserved DOI 10.1016/j.cub.2008.11.061 Report A Novel Vertebrate Eye Using Both Refractive and Reflective Optics Hans-Joachim Wagner,1 Ron H. Douglas,2,* mirror, and computer modeling indicates that this provides Tamara M. Frank,3 Nicholas W. Roberts,4,6 a well-focused image. This is the first report of an ocular and Julian C. Partridge5 image being formed in a vertebrate eye by a mirror. 1Anatomisches Institut Universita¨ tTu¨ bingen Results and Discussion O¨ sterbergstrasse 3 72074 Tu¨bingen The eyes of Dolichopteryx longipes have been described once Germany before [6]. However, relying on a single formalin-fixed spec- 2Henry Welcome Laboratory for Vision Sciences imen, this study was understandably incomplete and, in Department of Optometry and Visual Science places, erroneous. On a recent expedition, we caught a live City University specimen of this species, allowing a more thorough descrip- Northampton Square tion of its eyes. London EC1V 0HB UK General Ocular Morphology and Eyeshine 3Center for Ocean Exploration and Deep-Sea Research In dorsal view, D. longipes has two upward-pointing eyes, Harbor Branch Oceanographic Institute each with a dark swelling on its lateral face (Figures 1A and Florida Atlantic University 1B). Histological sectioning shows that each eye consists of 5600 U.S. 1 N two parts, largely separated by a dividing septum: the main, Fort Pierce, FL 34946 cylindrical, ‘‘tubular’’ eye (approximately 6 mm high and USA 4 mm wide) and a smaller, ovoid outgrowth from the lateral 4The Photon Science Institute wall of the cylinder (the diverticulum, approximately 2.6 mm School of Physics and Astronomy maximum height and 2.2 mm maximum width) (Figure 2). -
Optical Modeling of Schematic Eyes and the Ophthalmic Applications
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 8-2009 Optical Modeling of Schematic Eyes and the Ophthalmic Applications Bo Tan University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Atomic, Molecular and Optical Physics Commons Recommended Citation Tan, Bo, "Optical Modeling of Schematic Eyes and the Ophthalmic Applications. " PhD diss., University of Tennessee, 2009. https://trace.tennessee.edu/utk_graddiss/63 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Bo Tan entitled "Optical Modeling of Schematic Eyes and the Ophthalmic Applications." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Physics. James W. L. Lewis, Major Professor We have read this dissertation and recommend its acceptance: Ying-Ling Chen, Horace W. Crater, Christian Parigger, Ming Wang Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) To the Graduate Council: I am submitting herewith a dissertation written by Bo Tan entitled ―Optical modeling of schematic eyes and the ophthalmic applications.‖ I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of requirements for the degree of Doctor of Philosophy, with a major in Physics. -
Rays, Waves, and Scattering: Topics in Classical Mathematical Physics
chapter1 February 28, 2017 © Copyright, Princeton University Press. No part of this book may be distributed, posted, or reproduced in any form by digital or mechanical means without prior written permission of the publisher. Chapter One Introduction Probably no mathematical structure is richer, in terms of the variety of physical situations to which it can be applied, than the equations and techniques that constitute wave theory. Eigenvalues and eigenfunctions, Hilbert spaces and abstract quantum mechanics, numerical Fourier analysis, the wave equations of Helmholtz (optics, sound, radio), Schrödinger (electrons in matter) ... variational methods, scattering theory, asymptotic evaluation of integrals (ship waves, tidal waves, radio waves around the earth, diffraction of light)—examples such as these jostle together to prove the proposition. M. V. Berry [1] There is a theory which states that if ever anyone discovers exactly what the Universe is for and why it is here, it will instantly disappear and be replaced by something even more bizarre and inexplicable. There is another theory which states that this has already happened. Douglas Adams [155] Douglas Adams’s famous Hitchhiker trilogy consists of five books; coincidentally this book addresses the three topics of rays, waves, and scattering in five parts: (i) Rays, (ii) Waves, (iii) Classical Scattering, (iv) Semiclassical Scattering, and (v) Special Topics in Scattering Theory (followed by six appendices, some of which deal with more specialized topics). I have tried to present a coherent account of each of these topics by separating them insofar as it is possible, but in a very real sense they are inseparable. We are in effect viewing each phenomenon (e.g. -
Ophthalmic Optics
Handbook of Ophthalmic Optics Published by Carl Zeiss, 7082 Oberkochen, Germany. Revised by Dr. Helmut Goersch ZEISS Germany All rights observed. Achrostigmat®, Axiophot®, Carl Zeiss T*®, Clarlet®, Clarlet The publication may be repro• Aphal®, Clarlet Bifokal®, Clarlet ET®, Clarlet rose®, Clarlux®, duced provided the source is Diavari ®, Distagon®, Duopal ®, Eldi ®, Elta®, Filter ET®, stated and the permission of Glaukar®, GradalHS®, Hypal®, Neofluar®, OPMI®, the copyright holder ob• Plan-Neojluar®, Polatest ®, Proxar ®, Punktal ®, PunktalSL®, tained. Super ET®, Tital®, Ultrafluar®, Umbral®, Umbramatic®, Umbra-Punktal®, Uropal®, Visulas YAG® are registered trademarks of the Carl-Zeiss-Stiftung ® Carl Zeiss CR 39 ® is a registered trademark of PPG corporation. 7082 Oberkochen Optyl ® is a registered trademark of Optyl corporation. Germany Rodavist ® is a registered trademark of Rodenstock corporation 2nd edition 1991 Visutest® is a registered trademark of Moller-Wedel corpora• tion Reproduction and type• setting: SCS Schwarz Satz & Bild digital 7022 L.-Echterdingen Printing and production: C. Maurer, Druck und Verlag 7340 Geislingen (Steige) Printed in Germany HANDBOOK OF OPHTHALMIC OPTICS: Preface 3 Preface A decade has passed since the appearance of the second edition of the "Handbook of Ophthalmic Optics"; a decade which has seen many innovations not only in the field of ophthalmic optics and instrumentation, but also in standardization and the crea• tion of new terms. This made a complete revision of the hand• book necessary. The increasing importance of the contact lens in ophthalmic optics has led to the inclusion of a new chapter on Contact Optics. The information given in this chapter provides a useful aid for the practical work of the ophthalmic optician and the ophthalmologist.