PO Beam Waist Size and Location on the ISC Table
|
|
- Ashlyn Mitchell
- 6 years ago
- Views:
Transcription
1 LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T D 8/4/98 PO Beam Waist Sie and Location on the ISC Table Michael Smith Distribution of this draft: Table of Contents Index California Institute of Technology LIGO Project - MS 5-33 Pasadena CA 95 Phone (66) Fax (66) info@ligo.caltech.edu This is an internal working note of the LIGO Project. WWW: Massachusetts Institute of Technology LIGO Project - MS 0B-45 Cambridge, MA 039 Phone (67) Fax (67) info@ligo.mit.edu file H:\COS\ISC_tel_out.fm - printed August 4, 998
2 LIGO-T OVERVIEW The PO beam waist location on the ISC table can be varied by defocusing the ISC telescope. An optical schematic drawing of the PO beam optical train, which includes the 8X reflective telescope inside the vacuum housing and the 3.3X ISC telescope on the ISC optical table is shown in The input beam waist is inside the IFO, approximately 900 m from the PO telescope. The ISC telescope is separated from the PO telescope by approximately 3 m. The input beam waist is transformed by the lens train to an output beam waist of sie w 04, located in the vicinity of the ISC table at a distance 4 from the end of the ISC telescope. f +f d f 3 +f 4 + ISC w 0 w 0 w 03 w 04 w 04 L 3 L 4 L L 3X ISC telescope 8X PO telescope ISC Table Figure : Optical schematic of PO beam optical train The sie and location of the output beam waist can be determined by using Gaussian beam transformation theory. GAUSSIAN BEAM TRANSFORMATION THEORY An analysis of the dependence of the output beam waist and location on the defocusing of the ISC telescope was made using the following parameters.. Telescope Parameters PO Telescope primary focal length, f secondary focal length, f 54 mm mm page of 9
3 LIGO-T input beam waist position, input beam waist parameter, w 0 distance to ISC telescope, d ISC Telescope primary focal length, f 3 secondary focal length, f mm 36.4 mm 3000mm 58 mm mm.. Gaussian Beam Transformation Equations f f f. f π w 0. f w 0 w 0 w 0 f 0.5 w 0 w 0 f f f f f. w 0 f f w 0 w 0 w 0 f 0.5 page 3 of 9
4 LIGO-T w 03 w 0 3 d 3 f 3 f. 3 3 f 3 3 f 3 w 03 3 f 3 w 03 w 03 w 03 f w 04 w 03 4 ISC f 3 f 4 ISC 3 4 ISC f 4 ISC f 4 f ISC f 4 π w ISC f 4 w 04 ISC w 04 w 04 f 4 Raleigh range of ISC output, mm R ISC w 04 ISC 0.5 page 4 of 9
5 LIGO-T Results: Output Beam Waist Sie and Location The location of the ISC telescope output beam waist, as measured from the output lens, can be varied by defocusing the ISC telescope as shown in figure. The Rayleigh range associated with the output beam waist is also shown in figure. The output beam waist sie varies as the telescope is defocused, as shown in figure 3. The actual spot sie at the output of the ISC telescope is also plotted in figure 3. Beam waist position, and Rayleigh range, mm 4 ISC R ISC Rayleigh range beam waist position ISC Defocus, mm Figure : Beam waist position and Raleigh range versus ISC defocus, d=3000mm page 5 of 9
6 LIGO-T Gaussian beam radius, mm w 04 ISC w ISC 4 3 output spot sie beam waist sie ISC Defocus, mm Figure 3: Beam waist sie versus ISC defocus, d=3000mm.3. Locating the Far Field of the ISC Telescope It is desirable to minimie the effect of the position of the ISC telescope on the Guoy phase at the WFS detector, by placing the first Guoy lens of the WFS system in the far field of the ISC telescope output. This can be accomplished by defocusing the ISC telescope approximately -0.6 mm, which will place the apparent output beam waist at the location mm (refer to figure ). And since the Rayleigh range is mm, the output beam will be in the far field as it emerges from the ISC telescope. 3 ISC TELESCOPE DESIGN DETAILS 3. Optical Design Specification The optical design specification for the ISC telescope is shown in the optical schematic of figure 4. It will incorporate stock lenses, with AR coatings for 064 nm wavelength, as specified page 6 of 9
7 LIGO-T Mechanical Characteristics objective lens: part number nominal focal length diameter clear aperture center thickness edge thickness material Figure 4: ISC Telescope, optical schematic Edmund Scientific, p/n D mm mm 3 mm 7.5 mm 6.75 mm BK7/SF5 page 7 of 9
8 LIGO-T eyepiece lens: part number nominal focal length diameter clear aperture center thickness edge thickness material Edmund Scientific, p/n D mm mm 3 mm.5 mm 4.93 mm UV grade fused silica 3.3. Clear Aperture and Field of View Requirements The COS ISC telescope was designed with an optical axis displacement tolerance of +/- 8 mm, and a field-of-view tolerance of +/- 4x0^-4 rad. The total position shift and angular error in the COS pick off beam at the ISC table due to initial COC alignment errors, pump-down shifts, and long term stack drifts are estimated to be +/- 3 mm and 4x0^-3 rad; which exceed the design requirements of the ISC telescope. Therefore it will be necessary to direct the beam into the ISC telescope commensurate with the clear aperture and field-of-view design constraints. (See COS PDR sec , and Table 3) Mounting Configuration The ISC telescope lenses will be mounted in a simple focus tube configuration, as shown in figure 5. The focus tube must have a range of adjustment of -0.6 mm in order to place the output of the telescope in the far field, as described previously. See Locating the Far Field of the ISC Telescope on page 6. The telescope tube can be mounted to the ISC table with a standard tube mount fastened to an optical post, as shown. page 8 of 9
9 LIGO-T Dampened Rod Purchase Parts Adjustable Focus Tube - 40 UNS Thd. Approx Dia. ISC Telescope Full Sie ISC Telescope Figure 5: Mounting configuration, outline drawing for ISC telescope page 9 of 9
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T990088-01- D 10/14/99 COS IFO Alignment Procedure
More informationISC In-vacuum Gouy phase telescopes
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Technical Note LIGO-T1247-v3 211/3/5 ISC In-vacuum Gouy phase telescopes
More informationHeating Beam Pattern Optical Design CO2 Laser Thermal Compensation Bench
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO 4//4 Heating Beam Pattern Optical Design CO Laser Thermal Compensation Bench Michael Smith, David
More informationBeam Splitter Optical Surface Deformation due to Gravity
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO-T080233-01-D Advanced LIGO 22 Sep 2008 Beam Splitter Optical Surface Deformation due to Gravity
More informationLASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T960148-01- D Sep / 9 / 96 Maximum Current of the
More informationCase Study: Faraday Rotators in LIGO
Case Study: Faraday Rotators in LIGO Physics 208, Electro-optics Peter Beyersdorf Document info 1 Input Optics Overview Requirements for LIGO faraday isolator LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY
More informationDrag Wiping with Methanol vs First Contact
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO- T1000137_v3 LIGO Date: 08/08/2010 Drag Wiping with Methanol vs First Contact Margot Phelps, Liyuan
More informationCore Optics Support Conceptual Design
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T970072-01- D 4/2/97 Core Optics Support Conceptual
More informationNon-Linear Response of Test Mass to External Forces and Arbitrary Motion of Suspension Point
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY -LIGO- CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Technical Note LIGO-T980005-01- D 10/28/97 Non-Linear Response of Test
More informationSpatial Dependence of Force in the Initial LIGO OSEMs
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO - LIGO Scientific Collaboration LIGO - T75 - - I June Spatial Dependence of Force in the Initial LIGO OSEMs O d'arcy, P Fritschel Distribution of
More informationThe LIGO Observatory Environment
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO-T010074-00-D 06/28/2001 The LIGO Observatory Environment LIGO Systems Distribution of this document:
More informationValidation of the Source-Detector Simulation Formulation
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY -LIGO- CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Technical Note LIGO-T00152-00- E 7/1/0 Validation of the Source-Detector
More informationLIGO I mirror scattering loss by non smooth surface structure
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO-T070170-00-E LIGO July 26, 2007 LIGO I mirror scattering loss by non smooth surface structure Hiro
More informationLIGO On-line Documents July 1997
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T970089-05- P 7/22/97 LIGO On-line Documents July
More informationThermal Corrective Devices for Advanced Gravitational Wave Interferometers
Thermal Corrective Devices for Advanced Gravitational Wave Interferometers Marie Kasprzack, Louisiana State University 6 th October 2016 COMSOL Conference 2016 Boston 1 1. Advanced Gravitational Wave Detectors
More informationCore Optics Support Design Requirements Document
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T970071-02- D 2/25/98 Core Optics Support Design
More informationGravitational Waves & Precision Measurements
Gravitational Waves & Precision Measurements Mike Smith 1 -20 2 HOW SMALL IS THAT? Einstein 1 meter 1/1,000,000 3 1,000,000 smaller Wavelength of light 10-6 meters 1/10,000 4 10,000 smaller Atom 10-10
More informationLaser Optics-II. ME 677: Laser Material Processing Instructor: Ramesh Singh 1
Laser Optics-II 1 Outline Absorption Modes Irradiance Reflectivity/Absorption Absorption coefficient will vary with the same effects as the reflectivity For opaque materials: reflectivity = 1 - absorptivity
More informationLASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T070100-00- W 2007/05/17 Validation of the S5 V3
More informationWhy Use a Telescope?
1 Why Use a Telescope? All astronomical objects are distant so a telescope is needed to Gather light -- telescopes sometimes referred to as light buckets Resolve detail Magnify an image (least important
More informationall dimensions are mm the minus means meniscus lens f 2
TEM Gauss-beam described with ray-optics. F.A. van Goor, University of Twente, Enschede The Netherlands. fred@uttnqe.utwente.nl December 8, 994 as significantly modified by C. Nelson - 26 Example of an
More informationInstallation and testing of L1 PSL table legs
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO Laboratory / LIGO Scientific Collaboration LIGO April 15, 2012 Installation and testing of L1 PSL table legs R. DeSalvo, M. Rodruck, R. Savage,
More informationThe Treptow Giant Telescope in Berlin is the longest moveable refracting telescope on Earth. Some of its properties are summarised below:
Q1.(a) Draw a ray diagram for an astronomical refracting telescope in normal adjustment. Your diagram should show the paths of three non-axial rays passing through both lenses. Label the principal foci
More informationOptical Instruments. Chapter 25. Simple Magnifier. Clicker 1. The Size of a Magnified Image. Angular Magnification 4/12/2011
Optical Instruments Chapter 25 Optical Instruments Analysis generally involves the laws of reflection and refraction Analysis uses the procedures of geometric optics To explain certain phenomena, the wave
More informationOptics. Measuring the line spectra of inert gases and metal vapors using a prism spectrometer. LD Physics Leaflets P
Optics Spectrometer Prism spectrometer LD Physics Leaflets P5.7.1.1 Measuring the line spectra of inert gases and metal vapors using a prism spectrometer Objects of the experiment Adjusting the prism spectrometer.
More informationAssignment 3 Due September 27, 2010
Assignment 3 Due September 27, 2010 Text readings Stops section 5.3 Dispersing and Reflecting Prisms [sections 5.5.1 and 5.5.2] Optical systems section 5.7 Lens Aberrations [section 6.3] Be careful about
More informationA Question. Simple Magnifier. Magnification by a Lens 11/29/2011. The last lecture
The last lecture Exam: Final: Consult the website, especially room assignments. Makeup: Register with me today. Tea and Cookies: Tuesdays 5PM, NPB 2175 A Question Unpolarized light of intensity I goes
More informationAn alternative method to specify the degree of resonator stability
PRAMANA c Indian Academy of Sciences Vol. 68, No. 4 journal of April 2007 physics pp. 571 580 An alternative method to specify the degree of resonator stability JOGY GEORGE, K RANGANATHAN and T P S NATHAN
More information21. Propagation of Gaussian beams
1. Propagation of Gaussian beams How to propagate a Gaussian beam Rayleigh range and confocal parameter Transmission through a circular aperture Focusing a Gaussian beam Depth of field Gaussian beams and
More informationImplementing an Alignment Sensing and Control (ASC) System for the 40m Prototype Interferometer
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY -LIGO- CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Technical Note LIGO-T1300555-v1-2013/06/17 Implementing an Alignment
More informationUNIVERSITY OF SOUTHAMPTON
UNIVERSITY OF SOUTHAMPTON PHYS6012W1 SEMESTER 1 EXAMINATION 2012/13 Coherent Light, Coherent Matter Duration: 120 MINS Answer all questions in Section A and only two questions in Section B. Section A carries
More informationEfficient mode transformations of degenerate Laguerre Gaussian beams
Efficient mode transformations of degenerate Laguerre Gaussian beams Galina Machavariani, Amiel A. Ishaaya, Liran Shimshi, Nir Davidson, Asher A. Friesem, and Erez Hasman We present an approach for efficient
More informationPhysicsAndMathsTutor.com 1
PhysicsAndMathsTutor.com 1 1. The diagram shows the concave mirror of a Cassegrain reflecting telescope, together with the eyepiece lens. Complete the diagram of the telescope and mark on it the focal
More informationCHARA Meeting 2017 Pasadena, California
MORE AUTOMATION Laszlo Sturmann M7 ACTUATORS LAB. LASER ALIGNMENT TELESCOPE OPTICAL ALIGNMENT NEW ACTUATORS REMOTELY ACTUATED M7 MOUNT MOTIVATION THE PRECISION OF THE COUDE ALIGNMENT WAS NOT SUFFICIENT
More informationCosmography and Black Hole Spectroscopy by Coherent Synthesis of the Terrestrial and Space GW Antennae Network: Orbit Optimization
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY LIGO-F1500005 v1 2015/08/04 Cosmography and Black Hole Spectroscopy
More informationDiffraction I. Physics 2415 Lecture 37. Michael Fowler, UVa
Diffraction I Physics 2415 Lecture 37 Michael Fowler, UVa Today s Topics Michelson s interferometer The Michelson Morley experiment Single-slit diffraction Eye of a fly Angular resolution Michelson Interferometer
More informationExperiment 3 The Simple Magnifier, Microscope, and Telescope
Experiment 3 The Simple Magnifier, Microscope, and Telescope Introduction Experiments 1 and 2 dealt primarily with the measurement of the focal lengths of simple lenses and spherical s. The question of
More informationPHY410 Optics Exam #3
PHY410 Optics Exam #3 NAME: 1 2 Multiple Choice Section - 5 pts each 1. A continuous He-Ne laser beam (632.8 nm) is chopped, using a spinning aperture, into 500 nanosecond pulses. Compute the resultant
More informationAstronomy 203 practice final examination
Astronomy 203 practice final examination Fall 1999 If this were a real, in-class examination, you would be reminded here of the exam rules, which are as follows: You may consult only one page of formulas
More informationANALYSIS OF BURST SIGNALS IN LIGO DATA. Irena Zivkovic, Alan Weinstein
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY LIGO CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T010157-00-R 10/15/01 ANALYSIS OF BURST SIGNALS IN LIGO
More informationLAB DEMONSTRATION OF INTERFEROMETRIC
LAB DEMONSTRATION OF INTERFEROMETRIC MEASUREMENT USING A TEST PLATE AND CGH Presented to: Larry Stepp Eric Hansen The Association of Universities for Research in Astronomy, Inc. Tucson, AZ, 85726 Prepared
More informationTutorials. 1. Autocollimator. Angle Dekkor. General
Tutorials 1. Autocollimator General An autocollimator is a Precise Optical Instrument for measurement of small angle deviations with very high sensitivity. Autocollimator is essentially an infinity telescope
More informationCHAPTER IV INSTRUMENTATION: OPTICAL TELESCOPE
CHAPTER IV INSTRUMENTATION: OPTICAL TELESCOPE Outline: Main Function of Telescope Types of Telescope and Optical Design Optical Parameters of Telescope Light gathering power Magnification Resolving power
More informationTIE-43: Optical Properties of ZERODUR
PAGE 1/12 0 Introduction ZERODUR is a glass-ceramic material exhibiting a very low coefficient of thermal expansion The material is therefore used as a mirror substrate for astronomical telescopes or as
More informationManufacturing, Assembly, Integra5on and Tes5ng. 1. Lens and Mirror Manufacturing 2. Op6cal Tes6ng 3. Alignment 4. Tes6ng
Manufacturing, Assembly, Integra5on and Tes5ng 1. Lens and Mirror Manufacturing 2. Op6cal Tes6ng 3. Alignment 4. Tes6ng Introduc5on Detailed design finished and reviewed Tolerancing Alignment and test
More informationLASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY - LIGO - CALIFORNIA INSTITUTE OF TECHNOLOGY MASSACHUSETTS INSTITUTE OF TECHNOLOGY Document Type LIGO-T010126-00-E October 24th, 2001 Integration of mechanical
More informationPhysics 1252 Section Exam #1D
Thu, 09 February 2017 Name: Physics 1252 Section 36501 Exam #1D Instructions: This is a closed-book, closed-notes exam. You are allowed to use a clean print-out of your formula sheet, any scientific calculator,
More informationPhysics 1252 Section Exam #1E
Thu, 09 February 2017 Name: Physics 1252 Section 36501 Exam #1E Instructions: This is a closed-book, closed-notes exam. You are allowed to use a clean print-out of your formula sheet, any scientific calculator,
More informationConcave mirrors. Which of the following ray tracings is correct? A: only 1 B: only 2 C: only 3 D: all E: 2& 3
Concave mirrors Which of the following ray tracings is correct? A: only 1 B: only 2 C: only 3 D: all E: 2& 3 1 2 3 c F Point C: geometrical center of the mirror, F: focal point 2 Concave mirrors Which
More informationAuto collimator. Introduction. Objectives: Apparatus: Theory:
Auto collimator Introduction An autocollimator is an optical instrument that is used to measure small angles with very high sensitivity. As such, the autocollimator has a wide variety of applications including
More informationFEASIBILITY STUDY FOR THE FOCALISATION OF THE NEW 40m RADIOTELESCOPE OF CENTRO ASTRONÓMICO DE YEBES
Thirteenth international Symposium on Space Terahertz Technology, Harvard University, March 2002. FEASIBILITY STUDY FOR THE FOCALISATION OF THE NEW 40m RADIOTELESCOPE OF CENTRO ASTRONÓMICO DE YEBES E.
More informationNewtonian 17.5-inch Optical Tube Assembly
Newtonian 17.5-inch Optical Tube Assembly Kevin Phung 1, Jacob Hass 1, Victor Chen 2, Kevin Thompson 1, and Russell Genet 1, 3 1. California Polytechnic State University, San Luis Obispo, CA 2. University
More informationVacuum Kelvin Force Probe Research Richard Williams August 1st 2008
Vacuum Kelvin Force Probe Research Richard Williams August 1st 2008 Introduction Kelvin Force Probe Microscopy is an analytical method to measure the contact potential difference between a reference material
More informationDouble-slit Interference. Class 26: (ThT Q) Are both coherence and monochromaticity essential?
Double-slit Interference Class 26: (ThT Q) Are both coherence and monochromaticity essential? Exam 2 Discussion #9. Consider an arbitrary engine whose work output is connected to a Carnot engine running
More informationUse of computer generated holograms for alignment of complex null correctors
Use of computer generated holograms for alignment of complex null correctors Rene Zehnder, James H. Burge and Chunyu Zhao College of Optical Sciences, the University of Arizona 1630 E. University Blvd,
More informationTelescopes & Adaptive Optics. Roberto Ragazzoni INAF Astronomical Observatory of Padova
Telescopes & Adaptive Optics Roberto Ragazzoni INAF Astronomical Observatory of Padova PAST PAST FUTURE This is a simmetry line This object is drawn in a plane but it acctually reppresent a three dimensional
More informationAN OVERVIEW OF LIGO Adapted from material developed by Brock Wells Robert L. Olds Junior High School, Connell, WA August 2001
AN OVERVIEW OF LIGO Adapted from material developed by Brock Wells Robert L. Olds Junior High School, Connell, WA August 2001 The purpose of this guide is to provide background about the LIGO project at
More informationExperiment 3 The Simple Magnifier, Microscope, and Telescope
Experiment 3 The Simple Magnifier, Microscope, and Telescope Introduction Experiments 1 and 2 dealt primarily with the measurement of the focal lengths of simple lenses and spherical s. The question of
More informationGround- and Space-Based Telescopes. Dr. Vithal Tilvi
Ground- and Space-Based Telescopes Dr. Vithal Tilvi Telescopes and Instruments Astronomers use telescopes to gather light from distant objects and instruments to record the data Telescopes gather light
More informationSimulations of an etched spiral axial attenuation scheme for an on-axis reflecting telescope
Journal of Physics: Conference Series PAPER OPEN ACCESS Simulations of an etched spiral axial attenuation scheme for an on-axis reflecting telescope To cite this article: Aaron Spector and Guido Mueller
More informationMichelson Interferometer. crucial role in Einstein s development of the Special Theory of Relativity.
Michelson Interferometer The interferometer Michelson experiment Interferometer of Michelson and Morley played 0 a crucial role in Einstein s development of the Special Theory of Relativity. Michelson
More informationPhysics 1252 Sec.A Exam #1A
Physics 1252 Sec.A Exam #1A Instructions: This is a closed-book, closed-notes exam. You are allowed to use a clean print-out of your formula sheet, any scientific calculator, and a ruler. Do not write
More informationFaraday Isolator Performance at High Laser Power
Faraday Isolator Performance at High Laser Power R. M. Martin, V. Quetschke, A. Lucianetti, L. Williams, G. Mueller, D. H. Reitze, D. B. Tanner University of Florida Research supported by The National
More informationOptical Techniques for Gravitational-Wave Detection
Optical Techniques for Gravitational-Wave Detection M. Tacca Nikhef - Amsterdam Nikhef- 2017 July 14th Born in Novara (Italy) Introducing Myself PostDoc Fellow @ Nikhef (since July 2017) Laurea & PhD @
More informationThe Advanced LIGO detectors at the beginning of the new gravitational wave era
The Advanced LIGO detectors at the beginning of the new gravitational wave era Lisa Barsotti MIT Kavli Institute LIGO Laboratory on behalf of the LIGO Scientific Collaboration LIGO Document G1600324 LIGO
More informationA beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth.
Waves_P2 [152 marks] A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth. The beam is incident normally on a double slit. The distance between the slits
More informationCharacterization, Commissioning and Implementation of the Optical Lever System at Caltech s 40m Advanced LIGO Prototype Lab
LASER INTERFEROMETER GRAVITATIONAL WAVE OBSERVATORY --LIGO California Institute of Technology Massachusetts Institute of Technology Document Number: LIGO- T030231-00-R Date: 9/30/2003 Author: Naman Bhatt
More informationOPTICAL INSTRUMENTS VERY SHORT ANSWER QUESTIONS
OPTICAL INSTRUMENTS VERY SHORT ANSWER QUESTIONS Q-1. The difference in the focal lengths of the two lenses is larger in which case microscope or telescope? Q-2. What is the formula for angular magnification
More informationIMPRS: Ultrafast Source Technologies
IMPRS: Ultrafast Source Technologies Fran X. Kärtner & Thorsten Uphues, Bldg. 99, O3.097 & Room 6/3 Email & phone: fran.kaertner@cfel.de, 040 8998 6350 Thorsten.Uphues@cfel.de, 040 8998 706 Lectures: Tuesday
More informationGalileo Telescope Solar Viewer Joseph Hora, Elizabeth Hora 2017/09/18
Galileo Telescope Solar Viewer Joseph Hora, Elizabeth Hora 2017/09/18 17 7.75 5 2 1.5 3 2 1.5 Materials: (all dimensions in inches) 3x plywood sheet 17 x 7.75 x ½ 3x wood block cut from 2x4: 5 x 2 x 1.5
More informationAny first year text, sections on atomic structure, spectral lines and spectrometers
Physics 33 Experiment 5 Atomic Spectra References Any first year text, sections on atomic structure, spectral lines and spectrometers Any modern physics text, eg F.K. Richtmeyer, E.H. Kennard and J.N.
More informationDevelopment of a cryogenic compact interferometric displacement sensor
Development of a cryogenic compact interferometric displacement sensor Fabián E. Peña Arellano National Astronomical Observatory of Japan Outline of the presentation Motivation: local position sensor for
More informationOPSE FINAL EXAM Fall 2016 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.
CLOSED BOOK. Equation Sheet is provided. YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. ALL NUMERICAL ANSERS MUST HAVE UNITS INDICATED. (Except dimensionless units like
More information2.71. Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET
2.71 Final examination 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS Name: PLEASE RETURN THIS BOOKLET WITH YOUR SOLUTION SHEET(S) MASSACHUSETTS INSTITUTE OF TECHNOLOGY
More informationVersion 087 EX4 ditmire (58335) 1
Version 087 EX4 ditmire (58335) This print-out should have 3 questions. Multiple-choice questions ma continue on the next column or page find all choices before answering. 00 (part of ) 0.0 points A material
More informationKatherine Stewart. Telescopes. April 25, 2012
Katherine Stewart Telescopes April 25, 2012 History: Galileo created the first telescope in 1609.(Telescope History) Galileo s Original Telescope was composed of a concave objective lens and convex eyepiece
More informationPhysics 1302, Exam 3 Review
c V Andersen, 2006 1 Physics 1302, Exam 3 Review The following is a list of things you should definitely know for the exam, however, the list is not exhaustive. You are responsible for all the material
More informationAtomic and nuclear physics
Atomic and nuclear physics Atomic shell Normal Zeeman effect LEYBOLD Physics Leaflets Observing the normal Zeeman effect in transverse and longitudinal configuration Spectroscopy with a Fabry-Perot etalon
More informationPrac%ce Quiz 8. These are Q s from old quizzes. I do not guarantee that the Q s on this year s quiz will be the same, or even similar.
Prac%ce Quiz 8 These are Q s from old quizzes. I do not guarantee that the Q s on this year s quiz will be the same, or even similar. A laser beam shines vertically upwards. What laser power is needed
More informationPhysics 208 Exam 1 Oct. 3, 2007
1 Name: Student ID: Section #: Physics 208 Exam 1 Oct. 3, 2007 Print your name and section clearly above. If you do not know your section number, write your TA s name. Your final answer must be placed
More information6WDWXVRI/,*2. Laser Interferometer Gravitational-wave Observatory. Nergis Mavalvala MIT IAU214, August 2002 LIGO-G D
6WDWXVRI/,*2 Laser Interferometer Gravitational-wave Observatory Hanford, WA Livingston, LA Nergis Mavalvala MIT IAU214, August 2002 *UDYLWDWLRQDOZDYH,QWHUIHURPHWHUVWKHSULQ LSOH General Relativity (Einstein
More informationMANIPAL INSTITUTE OF TECHNOLOGY
SCHEME OF EVAUATION MANIPA INSTITUTE OF TECHNOOGY MANIPA UNIVERSITY, MANIPA SECOND SEMESTER B.Tech. END-SEMESTER EXAMINATION - MAY SUBJECT: ENGINEERING PHYSICS (PHY/) Time: 3 Hrs. Max. Marks: 5 Note: Answer
More informationThe Nulling Coronagraph Using a Nulling Interferometer for Planet Detection in Visible Light with a Single Aperture Telescope
Terrestrial Planet Finder The Nulling Coronagraph Using a Nulling Interferometer for Planet Detection in Visible Light with a Single Aperture Telescope Michael Shao, B. Martin Levine, Duncan Liu, J. Kent
More informationNATIONAL UNIVERSITY OF SINGAPORE DEPARTMENT OF PHYSICS ADVANCED PLACEMENT TEST (SAMPLE) INTRODUCTION TO THERMODYNAMICS AND OPTICS
NAIONAL UNIVERSIY OF SINGAPORE DEPARMEN OF PHYSICS ADVANCED PLACEMEN ES (SAMPLE) PC4 INRODUCION O HERMODYNAMICS AND OPICS MMM-YYYY----ime Allowed: Hours INSRUCIONS O CANDIDAES his paper contains five short
More informationExperimental Set-up of the 532nm Green Laser for the Measurement of the AC Stark Shift in a Cesium Fountain Clock
International Journal of Physics and Astronomy July-December 214, Vol. 2, No. 3 & 4, pp. 1-7 ISSN: 2372-4811 (Print), 2372-482X (Online) Copyright The Author(s). 214. All Rights Reserved. Published by
More informationDaily Alignment Procedure with 2 AO Wave Front Sensors
Daily Alignment Procedure with 2 AO Wave Front Sensors First Version Judit Sturmann Talk Outline AO at CHARA design scheme Before sky alignment Keeping the alignment during the night Lab and Telescope
More informationSupplemental material for Bound electron nonlinearity beyond the ionization threshold
Supplemental material for Bound electron nonlinearity beyond the ionization threshold 1. Experimental setup The laser used in the experiments is a λ=800 nm Ti:Sapphire amplifier producing 42 fs, 10 mj
More informationLecture 19 Optical MEMS (1)
EEL6935 Advanced MEMS (Spring 5) Instructor: Dr. Huikai Xie Lecture 19 Optical MEMS (1) Agenda: Optics Review EEL6935 Advanced MEMS 5 H. Xie 3/8/5 1 Optics Review Nature of Light Reflection and Refraction
More informationReverse technique for A1900
Reverse technique for A1900 v.9.10.270 from 02/03/16 1. LISE-type reverse file creation 2. Optics (1 1) 3. Optics (2 1) 4. Detector resolution for optics (1 1) 5. Contribution of straggling in wedge 6.
More informationPhysics 1212 Exam #1
Physics 1212 Exam #1 Instructions: This is a closed-book, closed-notes exam. You are allowed to use a clean print-out of your formula sheet, a non-progammable, non-algebra scientific calculator, and a
More informationThe science of light. P. Ewart
The science of light P. Ewart Oxford Physics: Second Year, Optics Parallel reflecting surfaces t images source Extended source path difference xcos 2t=x Fringes localized at infinity Circular fringe constant
More informationChapter Ray Optics and Optical Instrument
Chapter Ray Optics and Optical Instrument Q1. Focal length of a convex lens of refractive index 1.5 is 2 cm. Focal length of the lens when immersed in a liquid of refractive index of 1.25 will be [1988]
More informationLIGO s Thermal Noise Interferometer: Progress and Status
LIGO s Thermal Noise Interferometer: Progress and Status Eric Black LSC Meeting Review November 12, 2003 Ivan Grudinin, Akira Villar, Kenneth G. Libbrecht Thanks also to: Kyle Barbary, Adam Bushmaker,
More informationSingle Emitter Detection with Fluorescence and Extinction Spectroscopy
Single Emitter Detection with Fluorescence and Extinction Spectroscopy Michael Krall Elements of Nanophotonics Associated Seminar Recent Progress in Nanooptics & Photonics May 07, 2009 Outline Single molecule
More informationEfficient sorting of orbital angular momentum states of light
CHAPTER 6 Efficient sorting of orbital angular momentum states of light We present a method to efficiently sort orbital angular momentum (OAM) states of light using two static optical elements. The optical
More informationA faster, more accurate way of characterizing cube beamsplitters using the Agilent Cary 7000 Universal Measurement Spectrophotometer (UMS)
A faster, more accurate way of characterizing cube beamsplitters using the Agilent Cary 7000 Universal Measurement Spectrophotometer (UMS) Application note Materials Authors Travis Burt, Chris Colley,
More informationOptical Tweezers. The Useful Micro-Manipulation Tool in Research
Optical Tweezers The Useful Micro-Manipulation Tool in Research Student: Nikki Barron Class: Modern Physics/ Biophysics laboratory Advisor: Grant Allen Instructor: David Kleinfeld Date: June 15, 2012 Introduction
More informationWhat are the most important properties of a telescope? Chapter 6 Telescopes: Portals of Discovery. What are the two basic designs of telescopes?
Chapter 6 Telescopes: Portals of Discovery What are the most important properties of a telescope? 1. Light-collecting area: Telescopes with a larger collecting area can gather a greater amount of light
More informationOPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.
CLOSED BOOK. Equation Sheet is provided. YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT. ALL NUMERICAL ANSERS MUST HAVE UNITS INDICATED. (Except dimensionless units like
More informationAN OVERVIEW OF LIGO Brock Wells Robert L. Olds Junior High School, Connell, WA August 2001 LIGO
AN OVERVIEW OF LIGO Brock Wells Robert L. Olds Junior High School, Connell, WA August 2001 The purpose of this guide is to provide background about the LIGO project at the Hanford site. Hopefully this
More information