focusing optical elements and guides for neutron reflectometry experiences, projects and ideas
|
|
- Maximilian Black
- 5 years ago
- Views:
Transcription
1 PAUL SCHERRER INSTITUT Jochen Stahn Uwe Filges Laboratory for Neutron Scattering Laboratory for Developments and Methods focusing optical elements and guides for neutron reflectometry experiences, projects and ideas ESS Science Symposium Surface and Interface Reconstruction: A Challenge for Neutron Reflectometry , Bernried, Germany
2 people involved Emanouela Rantsiou Tobias Panzner Panos Korelis Uwe Filges McStas simulations Selene inspiration experiments Vincent Thominet Sibylle Spielmann Roman Bürge Marcel Schild Dieter Graf Jan Krebs PSI infrastructure Ursula Bengaard Hansen Wolfgang Kreuzpaintner Birgit Wiedemann Anette Vickery Sina Mayr ideas / discussions J. Stahn, Bernried Björgvin Hjörvarsson Marité Cardenas Beate Klösgen Rob Dalgliesh Frédéric Ott Phil Bentley Bob Cubitt Peter Böni Uwe Stuhr... thanx!
3 focusing J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
4 focusing: principles J. Stahn, Bernried focusing optics reshapes the phase space of a n-beam (an ensemble of neutrons) to a small spatial extent at a given position x θ conservation of states (neutrons) other conservative optics: mirror, non-focusing reflectors shading optics reshapes the phase space by restricting it in space (slit) or divergence (collimator) x θ loss of neutrons
5 focusing: principles focusing optics vs. slit optics J. Stahn, Bernried beam profile penumbra umbra beam profile umbra reflective / refractive optics slits
6 focusing: principles focusing optics vs. slit optics J. Stahn, Bernried beam profile penumbra umbra beam profile umbra reflective / refractive optics slits
7 focusing: principles J. Stahn, Bernried dimensions are freely scalable adjustable to TOF length sample environment spin-echo spatial needs available space... limited by aberration gravity
8 focusing: basic reflector shapes J. Stahn, Bernried parabolic parallel to convergent hyperbolic convergent to convergent elliptic divergent to convergent
9 focusing: full vs. half device J. Stahn, Bernried phase space homogeneity effective divergence y elliptic 2-sided ideal case θ "./mapes.dat"u 2:1:3 3 elliptic 1-sided
10 focusing: ballistic ellipse vs. half device J. Stahn, Bernried early reflections suffer the most from coma aberration multiple reflections non-convergent beam behind guide exit L.Cusssen et al.: NIM A 75, 121 (213) elliptic 2-sided large source / small entrance elliptic 1-sided
11 focusing: geometrical aberration J. Stahn, Bernried correction for coma aberration! a = 2 mm b = 4 mm accepted by 1 st guide intermediate image sample position width / mm θ / deg θ / deg θ / deg
12 focusing: chromatic aberration J. Stahn, Bernried due to gravity simulations (McStas) with (1mm) tapered guides (4m long, b/a =.22) in agreement with analytic calculations 1 I(z,λ) area normalised to 1 λ = Å 3Å 5Å 7Å 9Å I(z) z/mm
13 focusing Selene guide J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
14 focusing: Selene guide J. Stahn, Bernried point-to-point focusing with 2 subsequent elliptical reflectors for horizontal and vertical direction Selene Selene picture: ceiling painting in the Ny Carlsberg Glyptotek, København
15 focusing: Selene guide J. Stahn, Bernried footprint definition a luminous field diaphragm defines shape size orientation of the beam footprint on the sample to avoid over-illumination McSats simulations 1 A = 1 1mm 2 ω [.2,1.7 ] ω [6.1,7.6 ] avoid inhomogeneous field areas z/mm 5-5 raster the sample x/mm x/mm
16 focusing: Selene guide J. Stahn, Bernried decoupling of spot-size and divergence characteristic parameters guide length vs. max. wavelength divergence vs. min. wavelength 4a m λmax Å < 2 θ deg /λ min Å <.4
17 focusing: Selene guide operation modes θ deg J. Stahn, Bernried log 1 qz Å λ/å almost conventional reflectivity aperture = TOF defined foot-print off-specular reflectivity virtual source
18 focusing: Selene guide operation modes almost conventional reflectivity = TOF defined foot-print off-specular reflectivity θ deg λ/å (scanning) aperture J. Stahn, Bernried log 1 qz Å 1 λ-θ-encoding = TOF(θ) wider q z -range constant q/q virtual source
19 focusing: Selene guide operation modes almost conventional reflectivity = TOF defined foot-print off-specular reflectivity θ deg λ/å (scanning) aperture J. Stahn, Bernried log 1 qz Å 1 λ-θ-encoding = TOF(θ) wider q z -range constant q/q high-intensity specular reflectivity = TOF θ-dispersive split-second t-resolution screening of parameter space virtual source
20 experiences J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
21 experiences: Selene guide J. Stahn, Bernried prototype guide on slit = virtual source polariser chopper 1 st segment spin flipper 2 nd segment sample stage flight tube detector optical bench, 8m long in-situ sputtering & n-reflectometry B. Wiedemann, TU Munich
22 J. Stahn, Bernried 214 experiences: Selene guide prototype guide on Amor@PSI high-intensity specular reflectometry θ / deg reference.6 instrument Amor size time / spin 2 2 mm2 1 min θ / deg Si /Cu /Fe (6 monolayers) normalised sample λ/å log1 [ R (qz ) ] θ / deg sample 1.8 +i -1 i qz / A
23 experiences: logarithmic spiral J. Stahn, Bernried polariser, frame-overlap mirror can be applied to all convergent / divergent beams with small focus spot e.g. as analyser for any beam reflected on small or moderate-sized samples!
24 experiences: adaptive optics J. Stahn, Bernried condenser: parabolic deflector to generate a parallel beam parabola axis beam direction focal length beam width beam width & spot size divergence no collimator needed tunable adaptive parabola (convex) focal spot with 17µm reached (PSI, early version)
25 experiences: spectral analysis J. Stahn, Bernried using a multilayer monochromator 7 6 intensity α λ I(λ,θ) measured on Amor λ(θ)/å multilayer θ/deg double ML monochromator λ/å
26 projects J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
27 projects: Estia J. Stahn, Bernried ESS long pulse ( 3ms) high brilliance small moderator (3 12mm 2 ) operational in 22 reflectometers Freia liquid surfaces wide simultaneous q z -range Estia vertical scattering plane small (magnetic) samples??? GISANS
28 projects: Estia TOF reflectometer for the ESS horizontal scattering plane sample size < 1 5mm 2 feeder + Selene guide y x top view scattering plane J. Stahn, Bernried distance from moderator in m focusing guide system polariser virtual source fo-chopper source RF flipper sample detector aperture RF flipper analyser z x side view
29 J. Stahn, Bernried 214 projects: Estia comparison to prototype high-intensity specular reflectometry θ / deg Amor Estia size time / spin 2 2 mm2 1 min 1 2 mm2.2 s gain-factor: Si /Cu /Fe (6 monolayers) instrument θ / deg sample λ/å log1 [ R (qz ) ] θ / deg sample reference normalised 2 +i -1 i qz / A 1 reasons: brilliance of sources Amor guide (2%) sample size
30 projects: SINQ upgrade J. Stahn, Bernried Selene guide for Amor eventually at an other beam port horizontal and vertical scattering plane possible TOF and monochromatic mode (the project is in an early stage)
31 projects: Selene guide for spin-echo J. Stahn, Bernried MIEZE (NRSE) compatibility with Selene guide under investigation all trajectories have the same length G.Brandl, A.Chacón, R.Georgii, W.Häußler, et al. FRM II & TU Munich
32 ideas J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
33 ideas: astigmatic focusing J. Stahn, Bernried focus to the sample in the scattering sample plane focus to the sample detector in the scattering sample plane
34 ideas: astigmatic focusing J. Stahn, Bernried focus to the sample in the scattering sample plane specular off-specular intensity distributed over the detector focus to the sample detector in the scattering sample plane specular off-specular intensity concentrated along a line distributed over the detector strongly reduced background under specular signal
35 ideas: astigmatic focusing J. Stahn, Bernried focusing to the detector by shifting the focal point: hyperbolic deflector
36 ideas: astigmatic focusing J. Stahn, Bernried in combination with TOF and a chopper / scanning aperture / dispersive monochromator situation for one λ or t specular intensity concentrated on a small spot focusing GISANS configuration
37 discussion J. Stahn, Bernried focusing focusing Selene guide experiences projects ideas discussion
38 J. Stahn, Bernried 214 discussion focusing results in no gain in brilliance... a defined footprint... a clean beam homogeneous uni-modal angular or spatial distribution non-perfect optics reduction of resolution / transmission works best for small samples weak aberration 7.1
Monte Carlo simulation for adaptive optics
Monte Carlo simulation for adaptive optics R. Valicu 1, P. Böni 1,3, J. Stahn 2, U. Filges 2, T. Panzner 2, Y. Bodenthin 2, M. Schneider 2,3, C.Schanzer 3 1 Physik-Department E21, James-Franck-Strasse,
More informationLenses lens equation (for a thin lens) = (η η ) f r 1 r 2
Lenses lens equation (for a thin lens) 1 1 1 ---- = (η η ) ------ - ------ f r 1 r 2 Where object o f = focal length η = refractive index of lens material η = refractive index of adjacent material r 1
More informationDr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD (301) (301) fax
Dr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD 20723 (301) 953-6871 (301) 953-6670 fax Understand the instrument. Be able to convert measured counts/pixel on-orbit into
More informationOptics Vac Work MT 2008
Optics Vac Work MT 2008 1. Explain what is meant by the Fraunhofer condition for diffraction. [4] An aperture lies in the plane z = 0 and has amplitude transmission function T(y) independent of x. It is
More informationControl of Light. Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 2007
Control of Light Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 007 Spectro-radiometry Spectral Considerations Chromatic dispersion
More informationLecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization
Lecture 4 Recap of PHYS110-1 lecture Physical Optics - 4 lectures EM spectrum and colour Light sources Interference and diffraction Polarization Lens Aberrations - 3 lectures Spherical aberrations Coma,
More informationTowards 0.1 mm spatial resolution
Submitted for publication in ICNS Proceedings Towards 0.1 mm spatial resolution A. D. Stoica and X. L. Wang Spallation Neutron Source 701 Scarboro Road Oak Ridge National Laboratory Oak Ridge, TN 37831,
More informationChapter 36. Diffraction. Copyright 2014 John Wiley & Sons, Inc. All rights reserved.
Chapter 36 Diffraction Copyright 36-1 Single-Slit Diffraction Learning Objectives 36.01 Describe the diffraction of light waves by a narrow opening and an edge, and also describe the resulting interference
More informationSpectrographs. C. A. Griffith, Class Notes, PTYS 521, 2016 Not for distribution.
Spectrographs C A Griffith, Class Notes, PTYS 521, 2016 Not for distribution 1 Spectrographs and their characteristics A spectrograph is an instrument that disperses light into a frequency spectrum, which
More informationCondenser Optics for Dark Field X-Ray Microscopy
Condenser Optics for Dark Field X-Ray Microscopy S. J. Pfauntsch, A. G. Michette, C. J. Buckley Centre for X-Ray Science, Department of Physics, King s College London, Strand, London WC2R 2LS, UK Abstract.
More informationTEAMS National Competition High School Version Photometry 25 Questions
TEAMS National Competition High School Version Photometry 25 Questions Page 1 of 14 Telescopes and their Lenses Although telescopes provide us with the extraordinary power to see objects miles away, the
More informationDiffraction. Single-slit diffraction. Diffraction by a circular aperture. Chapter 38. In the forward direction, the intensity is maximal.
Diffraction Chapter 38 Huygens construction may be used to find the wave observed on the downstream side of an aperture of any shape. Diffraction The interference pattern encodes the shape as a Fourier
More informationExperiment 8 Wave Optics
Physics 263 Experiment 8 Wave Optics In this laboratory, we will perform two experiments on wave optics. 1 Double Slit Interference In two-slit interference, light falls on an opaque screen with two closely
More informationRay Optics I. Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex
Phys 531 Lecture 8 20 September 2005 Ray Optics I Last time, finished EM theory Looked at complex boundary problems TIR: Snell s law complex Metal mirrors: index complex Today shift gears, start applying
More informationSupplementary Figure 1 Optimum transmissive mask design for shaping an incident light to a desired
Supplementary Figure 1 Optimum transmissive mask design for shaping an incident light to a desired tangential form. (a) The light from the sources and scatterers in the half space (1) passes through the
More informationBasics of X-Area for image plates
Basics of X-Area for image plates Commercial software to process single-crystal and powder x-ray data from STOE image plates and PILATUS detectors Andrzej Grzechnik 1 & Karen Friese 2 1 Institute of Crystallography,
More informationLight: Geometric Optics
Light: Geometric Optics 23.1 The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization,
More informationChapter 32 Light: Reflection and Refraction. Copyright 2009 Pearson Education, Inc.
Chapter 32 Light: Reflection and Refraction Units of Chapter 32 The Ray Model of Light Reflection; Image Formation by a Plane Mirror Formation of Images by Spherical Mirrors Index of Refraction Refraction:
More informationChapter 23. Light Geometric Optics
Chapter 23. Light Geometric Optics There are 3 basic ways to gather light and focus it to make an image. Pinhole - Simple geometry Mirror - Reflection Lens - Refraction Pinhole Camera Image Formation (the
More informationMu lt i s p e c t r a l
Viewing Angle Analyser Revolutionary system for full spectral and polarization measurement in the entire viewing angle EZContrastMS80 & EZContrastMS88 ADVANCED LIGHT ANALYSIS by Field iris Fourier plane
More informationMID: Materials Imaging and Dynamics Instrument
MID: Materials Imaging and Dynamics Instrument A. Madsen 1,*, J. Hallmann 1, T. Roth 1, G. Ansaldi 1, W. Lu 1,2 1 European XFEL 2 Technische Universität Berlin * anders.madsen@xfel.eu XFEL User Meeting
More informationLIGHT & OPTICS. Fundamentals of Physics 2112 Chapter 34 1
LIGHT & OPTICS Fundamentals of Physics 22 Chapter 34 Chapter 34 Images. Two Types of Images 2. Plane Mirrors 3. Spherical Mirrors 4. Images from Spherical Mirrors 5. Spherical Refracting Surfaces 6. Thin
More informationLight: Geometric Optics
Light: Geometric Optics The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but
More informationAPPLICATION OF Ni/C-GÖBEL MIRRORS AS PARALLEL BEAM X-RAY OPTICS FOR Cu Ka AND Mo Ka RADIATION
Copyright(c)JCPDS-International Centre for Diffraction Data 2000,Advances in X-ray Analysis,Vol.43 212 APPLICATION OF Ni/C-GÖBEL MIRRORS AS PARALLEL BEAM X-RAY OPTICS FOR AND RADIATION T. Holz, R. Dietsch,
More informationAP Physics: Curved Mirrors and Lenses
The Ray Model of Light Light often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but is very useful for geometric
More informationDevelopment of EUV-Scatterometry for CD Characterization of Masks. Frank Scholze, Gerhard Ulm Physikalisch-Technische Bundesanstalt, Berlin, Germany
Development of EUV-Scatterometry for CD Characterization of Masks PB Frank Scholze, Gerhard Ulm Physikalisch-Technische Bundesanstalt, Berlin, Germany Jan Perlich, Frank-Michael Kamm, Jenspeter Rau nfineon
More informationTEAMS National Competition Middle School Version Photometry 25 Questions
TEAMS National Competition Middle School Version Photometry 25 Questions Page 1 of 13 Telescopes and their Lenses Although telescopes provide us with the extraordinary power to see objects miles away,
More informationSimple Spectrograph. grating. slit. camera lens. collimator. primary
Simple Spectrograph slit grating camera lens collimator primary Notes: 1) For ease of sketching, this shows a transmissive system (refracting telescope, transmission grating). Most telescopes use a reflecting
More informationLight: Geometric Optics (Chapter 23)
Light: Geometric Optics (Chapter 23) Units of Chapter 23 The Ray Model of Light Reflection; Image Formed by a Plane Mirror Formation of Images by Spherical Index of Refraction Refraction: Snell s Law 1
More informationPhys102 Lecture 21/22 Light: Reflection and Refraction
Phys102 Lecture 21/22 Light: Reflection and Refraction Key Points The Ray Model of Light Reflection and Mirrors Refraction, Snell s Law Total internal Reflection References 23-1,2,3,4,5,6. The Ray Model
More information2011 Optical Science & Engineering PhD Qualifying Examination Optical Sciences Track: Advanced Optics Time allowed: 90 minutes
2011 Optical Science & Engineering PhD Qualifying Examination Optical Sciences Track: Advanced Optics Time allowed: 90 minutes Answer all four questions. All questions count equally. 3(a) A linearly polarized
More informationWinmeen Tnpsc Group 1 & 2 Self Preparation Course Physics UNIT 9. Ray Optics. surface at the point of incidence, all lie in the same plane.
Laws of reflection Physics UNIT 9 Ray Optics The incident ray, the reflected ray and the normal drawn to the reflecting surface at the point of incidence, all lie in the same plane. The angle of incidence
More informationChapter 36. Image Formation
Chapter 36 Image Formation Apr 22, 2012 Light from distant things We learn about a distant thing from the light it generates or redirects. The lenses in our eyes create images of objects our brains can
More informationLight Tec Scattering measurements guideline
Light Tec Scattering measurements guideline 1 2 Light Tec Locations REFLET assembling plant, Aix-en-Provence, France Light Tec GmbH, Munich, Germany German office Light Tec Sarl, Hyères, France Main office
More informationFRED Slit Diffraction Application Note
FRED Slit Diffraction Application Note The classic problem of diffraction through a slit finds one of its chief applications in spectrometers. The wave nature of these phenomena can be modeled quite accurately
More informationEfficient wave-optical calculation of 'bad systems'
1 Efficient wave-optical calculation of 'bad systems' Norman G. Worku, 2 Prof. Herbert Gross 1,2 25.11.2016 (1) Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany (2)
More informationChemistry Instrumental Analysis Lecture 6. Chem 4631
Chemistry 4631 Instrumental Analysis Lecture 6 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.
More informationAP* Optics Free Response Questions
AP* Optics Free Response Questions 1978 Q5 MIRRORS An object 6 centimeters high is placed 30 centimeters from a concave mirror of focal length 10 centimeters as shown above. (a) On the diagram above, locate
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 42 Review Spring 2013 Semester Matthew Jones Final Exam Date:Tuesday, April 30 th Time:1:00 to 3:00 pm Room: Phys 112 You can bring two double-sided pages of
More informationPHYSICS 213 PRACTICE EXAM 3*
PHYSICS 213 PRACTICE EXAM 3* *The actual exam will contain EIGHT multiple choice quiz-type questions covering concepts from lecture (16 points), ONE essay-type question covering an important fundamental
More informationProgress of the Thomson Scattering Experiment on HSX
Progress of the Thomson Scattering Experiment on HSX K. Zhai, F.S.B. Anderson, D.T. Anderson HSX Plasma Laboratory, UW-Madison Bill Mason PSL, UW-Madison, The Thomson scattering system being constructed
More informationFinal Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus
Physics 42200 Waves & Oscillations Lecture 40 Review Spring 206 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 2 You can bring one double-sided pages of notes/formulas.
More informationLENSES DDC TECHNOLOGIES
LENSES Optical Glass Plano-convex Lenses... 2 Optical Glass Plano-concave Lenses... 3 Optical Glass Bi-convex Lenses... 4 Optical Glass Bi-concave Lenses... 5 Fused Silica Plano-convex Lenses... 6 Fused
More informationGrazing Angle 2 Theta Phase Analysis
Page 1 of 7 Grazing Angle 2 Theta Phase Analysis 1. Log into the User Log System on the SMIF web site Hardware Setup X-Ray Tube The line focus configuration of the x-ray tube is used. This is the default
More informationSecond Year Optics 2017 Problem Set 1
Second Year Optics 2017 Problem Set 1 Q1 (Revision of first year material): Two long slits of negligible width, separated by a distance d are illuminated by monochromatic light of wavelength λ from a point
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 40 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.
More informationRay optics! Postulates Optical components GRIN optics Matrix optics
Ray optics! Postulates Optical components GRIN optics Matrix optics Ray optics! 1. Postulates of ray optics! 2. Simple optical components! 3. Graded index optics! 4. Matrix optics!! From ray optics to
More informationCrystal Quality Analysis Group
Crystal Quality Analysis Group Contents Contents 1. Overview...1 2. Measurement principles...3 2.1 Considerations related to orientation and diffraction conditions... 3 2.2 Rocking curve measurement...
More informationOptical design of COrE+
Optical design of COrE+ Karl Young November 23, 2015 The optical designs for COrE+ were made by Darragh McCarthy and Neil Trappe at Maynooth University and Karl Young and Shaul Hanany at University of
More informationBasic optics. Geometrical optics and images Interference Diffraction Diffraction integral. we use simple models that say a lot! more rigorous approach
Basic optics Geometrical optics and images Interference Diffraction Diffraction integral we use simple models that say a lot! more rigorous approach Basic optics Geometrical optics and images Interference
More informationLight Tec Scattering measurements guideline
Light Tec Scattering measurements guideline 1 Our Laboratory Light Tec is equipped with a Photometric Laboratory (a dark room) including: Goniophotometers: REFLET 180S. High specular bench (10 meters),
More informationISO INTERNATIONAL STANDARD. Particle size analysis Laser diffraction methods. Analyse granulométrique Méthodes par diffraction laser
INTERNATIONAL STANDARD ISO 13320 First edition 2009-10-01 Corrected version 2009-12-01 Particle size analysis Laser diffraction methods Analyse granulométrique Méthodes par diffraction laser Reference
More informationChapter 38. Diffraction Patterns and Polarization
Chapter 38 Diffraction Patterns and Polarization Diffraction Light of wavelength comparable to or larger than the width of a slit spreads out in all forward directions upon passing through the slit This
More informationLight Tec Scattering measurements guideline
Light Tec Scattering measurements guideline 1 Our Laboratory Light Tec is equipped with a Photometric Laboratory (a dark room) including: Goniophotometers: REFLET180s. High specular bench (10 meters),
More informationTo determine the wavelength of laser light using single slit diffraction
9 To determine the wavelength of laser light using single slit diffraction pattern 91 Apparatus: Helium-Neon laser or diode laser, a single slit with adjustable aperture width, optical detector and power
More information2. THE PHYSICS OF DIFFRACTION GRATINGS
Diffraction Grating Handbook - Chapter 1 2. THE PHYSICS OF DIFFRACTION GRATINGS PREVIOUS CHAPTER NEXT CHAPTER Copyright 2002, Thermo RGL, All Rights Reserved TABLE OF CONTENTS 2.1. THE GRATING EQUATION
More informationScattering measurements. Guidelines for measurements service
Scattering measurements Guidelines for measurements service 1 Content Introduction Light Tec Presentation Instruments availalable. Scattering measurements Refelctors Diffusers Colors issuses Volume Scattering
More informationReflective Illumination for DMS 803 / 505
APPLICATION NOTE // Dr. Michael E. Becker Reflective Illumination for DMS 803 / 505 DHS, SDR, VADIS, PID & PLS The instruments of the DMS 803 / 505 series are precision goniometers for directional scanning
More informationWir schaffen Wissen heute für morgen. Paul Scherrer Institut X10SA Partner Training Workshop 2014 (New) Features at X10SA
Wir schaffen Wissen heute für morgen Paul Scherrer Institut X10SA Partner Training Workshop 2014 (New) Features at X10SA PSI, 1. April 2014 Major Developments Since Last Training (2009) 2010 2011 2012
More informationDynamical Theory of X-Ray Diffraction
Dynamical Theory of X-Ray Diffraction ANDRE AUTHIER Universite P. et M. Curie, Paris OXFORD UNIVERSITY PRESS Contents I Background and basic results 1 1 Historical developments 3 1.1 Prologue 3 1.2 The
More informationANOMALOUS SCATTERING FROM SINGLE CRYSTAL SUBSTRATE
177 ANOMALOUS SCATTERING FROM SINGLE CRYSTAL SUBSTRATE L. K. Bekessy, N. A. Raftery, and S. Russell Faculty of Science, Queensland University of Technology, GPO Box 2434, Brisbane, Queensland, Australia
More informationPolarizers. Laser Polarizers Broadband Polarizing Beamsplitting Cubes 78 Narrowband Polarizing Beamsplitting Cubes 79
Prisms Introduction to Right Angle Prisms 72 Quality Right Angle Prisms 73 Laboratory Quality Right Angle Prisms 73 Equilateral Prisms 74 Wedge Prisms 75 Anamorphic Prism Pair 75 Penta Prisms 76 Dove Prisms
More informationGeometrical Optics INTRODUCTION. Wave Fronts and Rays
Geometrical Optics INTRODUCTION In this experiment, the optical characteristics of mirrors, lenses, and prisms will be studied based on using the following physics definitions and relationships plus simple
More informationX-rays are electro-magnetic radiation
X-rays are electro-magnetic radiation Just like visible light, X-rays are waves - cos[ 2π ( x / λ ft)] X-rays travel at the speed of light (c) Quantum Mechanics gives the energy of an X-ray photon c =
More informationMichelson Interferometer
Michelson Interferometer The Michelson interferometer uses the interference of two reflected waves The third, beamsplitting, mirror is partially reflecting ( half silvered, except it s a thin Aluminum
More informationE x Direction of Propagation. y B y
x E x Direction of Propagation k z z y B y An electromagnetic wave is a travelling wave which has time varying electric and magnetic fields which are perpendicular to each other and the direction of propagation,
More informationaxis, and wavelength tuning is achieved by translating the grating along a scan direction parallel to the x
Exponential-Grating Monochromator Kenneth C. Johnson, October 0, 08 Abstract A monochromator optical design is described, which comprises a grazing-incidence reflection and two grazing-incidence mirrors,
More informationLight Tec Scattering measurements guideline
Light Tec Scattering measurements guideline 1 Our Laboratory Light Tec is equipped with a Photometric Laboratory (a dark room) including: Goniophotometers: REFLET 180S. High specular bench (10 meters),
More informationPart Images Formed by Flat Mirrors. This Chapter. Phys. 281B Geometric Optics. Chapter 2 : Image Formation. Chapter 2: Image Formation
Phys. 281B Geometric Optics This Chapter 3 Physics Department Yarmouk University 21163 Irbid Jordan 1- Images Formed by Flat Mirrors 2- Images Formed by Spherical Mirrors 3- Images Formed by Refraction
More informationRepresenting the World
Table of Contents Representing the World...1 Sensory Transducers...1 The Lateral Geniculate Nucleus (LGN)... 2 Areas V1 to V5 the Visual Cortex... 2 Computer Vision... 3 Intensity Images... 3 Image Focusing...
More informationRay Optics. Lecture 23. Chapter 23. Physics II. Course website:
Lecture 23 Chapter 23 Physics II Ray Optics Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Let s finish talking about a diffraction grating Diffraction Grating Let s improve (more
More informationUNIT VI OPTICS ALL THE POSSIBLE FORMULAE
58 UNIT VI OPTICS ALL THE POSSIBLE FORMULAE Relation between focal length and radius of curvature of a mirror/lens, f = R/2 Mirror formula: Magnification produced by a mirror: m = - = - Snell s law: 1
More informationDiffraction. Introduction: Diffraction is bending of waves around an obstacle (barrier) or spreading of waves passing through a narrow slit.
Introduction: Diffraction is bending of waves around an obstacle (barrier) or spreading of waves passing through a narrow slit. Diffraction amount depends on λ/a proportion If a >> λ diffraction is negligible
More informationBasic Polarization Techniques and Devices 1998, 2003 Meadowlark Optics, Inc
Basic Polarization Techniques and Devices 1998, 2003 Meadowlark Optics, Inc This application note briefly describes polarized light, retardation and a few of the tools used to manipulate the polarization
More informationA 4. An electromagnetic wave travelling through a transparent medium is given by y. in S units. Then what is the refractive index of the medium?
SECTION (A) : PRINCIPLE OF SUPERPOSITION, PATH DIFFERENCE, WAVEFRONTS, AND COHERENCE A 1. Two sources of intensity I & 4I are used in an interference experiment. Find the intensity at points where the
More informationSpectrograph overview:
High performance measurement systems Monochromator Family Gilden Photonics offers a range of integrated optical wavelength solutions in customized designs, OEM design, manufacturing and value added resell
More informationMicro Structures Design of OLED Tail Lamp Abstract 1. Introduction
Micro Structures Design of OLED Tail Lamp Yao-Min Ho, Jih-Tao Hsu Automotive Research Testing Center No.6, Lugong S.7th Rd.,Lugang,Changhua County 50544,Taiwan(R.O.C) E-mail: yaomin@artc.org.tw Abstract
More informationA systematic approach to the analysis of polarisation-sensitive reflectors
A systematic approach to the analysis of polarisation-sensitive reflectors Hans-Henrik Viskum TICRA Læderstræde 34, 2. DK-1201 Copenhagen K Denmark hhv@ticra.com ABSTRACT The analysis of a polarisation-sensitive
More informationTwo slit interference - Prelab questions
Two slit interference - Prelab questions 1. Show that the intensity distribution given in equation 3 leads to bright and dark fringes at y = mλd/a and y = (m + 1/2) λd/a respectively, where m is an integer.
More informationWave Optics. April 11, 2014 Chapter 34 1
Wave Optics April 11, 2014 Chapter 34 1 Announcements! Exam tomorrow! We/Thu: Relativity! Last week: Review of entire course, no exam! Final exam Wednesday, April 30, 8-10 PM Location: WH B115 (Wells Hall)
More informationRay Optics. Lecture 23. Chapter 34. Physics II. Course website:
Lecture 23 Chapter 34 Physics II Ray Optics Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Today we are going to discuss: Chapter 34: Section 34.1-3 Ray Optics Ray Optics Wave
More informationNicholas J. Giordano. Chapter 24. Geometrical Optics. Marilyn Akins, PhD Broome Community College
Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 24 Geometrical Optics Marilyn Akins, PhD Broome Community College Optics The study of light is called optics Some highlights in the history
More information4. A bulb has a luminous flux of 2400 lm. What is the luminous intensity of the bulb?
1. Match the physical quantities (first column) with the units (second column). 4. A bulb has a luminous flux of 2400 lm. What is the luminous intensity of the bulb? (π=3.) Luminous flux A. candela Radiant
More informationPhysics 214 Midterm Fall 2003 Form A
1. A ray of light is incident at the center of the flat circular surface of a hemispherical glass object as shown in the figure. The refracted ray A. emerges from the glass bent at an angle θ 2 with respect
More informationdq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ =
Radiometry (From Intro to Optics, Pedrotti -4) Radiometry is measurement of Emag radiation (light) Consider a small spherical source Total energy radiating from the body over some time is Q total Radiant
More informationStevens High School AP Physics II Work for Not-school
1. Gravitational waves are ripples in the fabric of space-time (more on this in the next unit) that travel at the speed of light (c = 3.00 x 10 8 m/s). In 2016, the LIGO (Laser Interferometry Gravitational
More information4. Recommended alignment procedure:
4. Recommended alignment procedure: 4.1 Introduction The described below procedure presents an example of alignment of beam shapers Shaper and Focal- Shaper (F- Shaper) with using the standard Shaper Mount
More informationChapter 4 - Diffraction
Diffraction is the phenomenon that occurs when a wave interacts with an obstacle. David J. Starling Penn State Hazleton PHYS 214 When a wave interacts with an obstacle, the waves spread out and interfere.
More informationLED Evenement 2014 Spectroscopy - Straylight. Avantes BV Apeldoorn, The Netherlands
LED Evenement 2014 Spectroscopy - Straylight Avantes BV Apeldoorn, The Netherlands Content: - Company - Spectroscopy - Spectrometer measuring light - Straylight - How to prevent - Why - conclusion Introduction
More informationNon-line-of-sight imaging
Non-line-of-sight imaging http://graphics.cs.cmu.edu/courses/15-463 15-463, 15-663, 15-862 Computational Photography Fall 2017, Lecture 25 Course announcements Homework 6 will be posted tonight. - Will
More informationCharacterizing x-ray mirrors in reciprocal space
Characterizing x-ray mirrors in reciprocal space Preliminary results from the NIST X-ray Optics Evaluation Double-Crystal Diffractometer D.L. Gil, D. Windover, J.P. Cline, A. Henins National Institute
More informationDiffuse Terahertz Reflection Imaging using Quantum Cascade Lasers
Diffuse Terahertz Reflection Imaging using Quantum Cascade Lasers P. Dean, S. P. Khanna, S. Chakraborty, M. Lachab, A. G. Davies, E. H, Linfield Institute of Microwaves and Photonics School of Electronic
More informationThroughput of an Optical Instrument II: Physical measurements, Source, Optics. Q4- Number of 500 nm photons per second generated at source
Throughput of an Optical Instrument II: Physical measurements, Source, Optics Question- Value Q1- Percent output between 450-550 nm by mass Answer (w/ units) Q2- Energy in J of a 500 nm photon Q3- Flux
More informationRefractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different
Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from
More informationMaintenance Package Measurement
Maintenance Package Measurement Contents Contents 1. Package measurement flow...1 2. Measurement procedures...3 2.1 Startup... 3 2.2 Hardware setup... 4 2.3 Setting Package measurement conditions... 7
More informationWaves & Oscillations
Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2013 Semester Matthew Jones Final Exam Date:Tuesday, April 30 th Time:1:00 to 3:00 pm Room: Phys 112 You can bring two double-sided pages of
More informationRay Optics. Physics 11. Sources of Light Rays: Self-Luminous Objects. The Ray Model of Light
Physics 11 Ray Optics Ray Model of Light Reflection Plane Mirrors Spherical Mirrors Ray Tracing Images from a Concave Mirror Images from a Convex Mirror Slide 18-3 The Ray Model of Light Sources of Light
More informationChapter 35 &36 Physical Optics
Chapter 35 &36 Physical Optics Physical Optics Phase Difference & Coherence Thin Film Interference 2-Slit Interference Single Slit Interference Diffraction Patterns Diffraction Grating Diffraction & Resolution
More informationQUICK X-RAY REFLECTIVITY OF SPHERICAL SAMPLES
Copyright JCPDS-International Centre for Diffraction Data 2013 ISSN 1097-0002 10 QUICK X-RAY REFLECTIVITY OF SPHERICAL SAMPLES Krassimir Stoev 1, Kenji Sakurai 2,3 1 AECL Chalk River Laboratories, Chalk
More information