DOCSLIB.ORG

What Next with the Candela

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
What Next with the Candela What next with the candela 20th Meeting of the NMI Directors . Introduction of defining constant for photometry, Kcd luminous efficacy of monochromatic radiation of frequency 540 × 1012 Hz . Reformulation of definition of the candela ‐ (not a redefinition), to bring it in explicit constant form: www.bipm.org 2 Mole 71 Candela 79 Metre 83 2 1 3 Jeff Wall, Invisible Man Km Kcd The luminous efficacy of monochromatic 12 radiation of frequency 540 × 10 Hz, Kcd, is 683 lm/W. www.bipm.org 3 • Kcd makes a direct link between photometric and radiometric quantities for monochromatic radiation of frequency 540 THz flux illuminance intensity luminance lm ↔ W lx ↔ W∙m‐2 cd ↔ W∙sr‐1 cd∙m‐2 ↔ W∙sr‐1∙m‐2 Kcd Kcd Kcd Kcd • Mise en pratique for the definition of the candela in the SI (20 May 2019) • BIPM report 05/2019: Principles governing photometry (20 May 2019) • Appendix 3 Units for photochemical and photobiological quantities (20 May 2019) www.bipm.org 4 Photometry Kyle Bean – Interconnected senses Warhol, Marilyn www.bipm.org Monroe(1967) 5 Photometry Photometry is the science of the measurement of light, in terms of its perceived brightness to the human eye. To do photometry, you need : eyes brain light stimulus www.bipm.org 6 Photometry light source material light stimulus www.bipm.org 7 Measurement of perceptive quantities Challenge The measurand is not accessible by the measuring instrument Measurand Object www.bipm.org 8 Measurement of perceptive quantities Is stimulus 1 = stimulus 2 ? Stimulus Stimulus 1 2 www.bipm.org 9 Measurement of visual quantities Photometry deals with visual quantities. The measurand is not accessible by the measuring instrument The measurand may vary from an observer to another Visual quantity Object www.bipm.org 10 Vision and V() curve Human eye Lens Retina Fovea Rod Optical nerve Cone www.bipm.orgSource : ??? 1111 Vision and V() curve Cones (L M S) We have 3 family of cones. Light that reaches the retina generates 3 signals in the cones, that depend upon the wavelength S( ) L() Fundamentale sensitivity S() max 440 nm Sensibilité fondamentale Sensibilité M() M() max 540 nm L() max 570 nm 400 nm 700 nm www.bipm.org 1212 Vision and V() curve Individual variations We don’t have the same repartition of cones, but the visual system adjusts the sensitivity by adapting the gain Hofer, Carroll, Neitz, Neitz, Williams, JNeuroscience 2005 www.bipm.org 1313 Vision and V() curve CIE Photometric strandard observer 6th session of CIE, Geneva, 1924 K. S. Gibson : Visibility function 272 observers (UK, Japan, US) www.bipm.org 1414 Vision and V() curve CIE Photometric strandard observer V(λ) curve λmax = 555 nm 1,0 0,8 0,6 0,4 0,2 0 400 500555 600 700 (nm) www.bipm.org 15 Many agreed human visual response function (mesopic & 10°) www.bipm.org 16 Observers Female / Male Young / Old Naïve / Expert Colour blind? Vision corrected Morning / Afternoon ….. www.bipm.org 17 Photometry deals with visual quantities. The measurand is not accessible by the measuring instrument The measurand may vary from an observer to another Visual quantity Object www.bipm.org 18 The measurand may vary from an observer to an other Elaine Moynihan Lisle Miraï www.bipm.org Monet 19 Photometry describes the effects of visible light on the human eye, in terms of brightness and colour www.bipm.org 20 Towards the candela Visual comparisons What is the reference? UK Parliamentary Candle (1860) Extracted from “manipulation de physique” A. Leduc, 1895 1854 www.bipm.org 21 Towards the candela First standard Standard lamps Carcel Lamp Hefner Lamp Vernon Harcourt lamp © Cnam - Musée © PTB © NIST 1890 www.bipm.org 22 Towards the candela 1900 : the « black body », the ideal standard Radiance from the black body depends only of its temperature 2hc2 1 Lλ(λ,T) = λ5 e hc/(λkT) − 1 with : wavelength of the radiation T, black body temperature c, speed of light Photo collection particulière D. J. Lovell h, Planck constant Max Planck k, Boltzmann constant www.bipm.org 23 Towards the candela Freezing temperature of Platinium «“The candela is the luminous intensity, in the perpendicular direction, of a surface of 1/600 000 square metre of a black body at the temperature of freezing platinum under a pressure of 101 325 newtons per square metre.”» XIIIème CGPM, 1968 If the feezing platinum temperature varies, the radiation emitted by the black body varies and the candela varies !! Temperature [°C] 1775 0,23% 1770 1765 1940 1960 1980 2000 2020 years www.bipm.org 24 Radiometry, a new way for the candela Radiometry to rescue photometry Radiometry is the science of measurement of radiant energy (including light) in terms of absolute power. Radiometric techniques characterize the distributionoftheradiant power according to the wavelength. www.bipm.org 25 Radiometry, a new way for the candela LIGHT Electromagnetic waves with a wavelength between 380 nm and 780 nm 380 nm 780 nm Violet Blue Green Yellow Orange Red www.bipm.org 26 Radiometry, a new way for the candela Spectral power distribution of light sources Spectral power distribution describes the light spectrum of a light source It shows which radiations are present, at which wavelength, in which proportion. He‐Ne Laser White light source Power Power (W) (W) Wavelenght (nm) Wavelength (nm) www.bipm.org 27 Radiometry, a new way for the candela Progress in radiometry Radiometry allows measurement of 1,000% optical power at each wavelength 0,100% 0,010% 0,001% Relative standard uncertainty 1900 1920 1940 1960 1980 2000 2020 2040 2010 ‐> today www.bipm.org 28 Radiometry, a new way for the candela cryogenic radiometer 0,6 0,5 Absolute measurement on laser is good. 0,4 But transfer to incoherent light needs improvement 0,3 0,2 0,1 Dispersion and uncertainty / % 0 350 450 550 650 750 850 950 nm ‐0,1 www.bipm.org 29 Sensitivity curve of human eye www.bipm.org 30 Radiometry, a new way for the candela the new way… I [cd] E [lx] d I E = «The candela is the luminous intensity, in the 2 perpendicular direction, of a surface of T [K] d 1/600 000 square meter of a black body at the temperature of freezing platinum» 1948 : IXème CGPM www.bipm.org 31 Radiometry, a new way for the candela the new way… I [cd] diaphragm E [lx] S d P [W] I E = «The candela is the luminous intensity, in the 2 perpendicular direction, of a light source that d generates an illuminance of 1 lx at 1m distance, that is accessed by radiometry xxx : xxxème CGPM www.bipm.org 3232 Vision and V() curve CIE Photometric strandard observer V(λ) curve λmax = 555 nm 1,0 0,8 0,6 0,4 0,2 0 400 500555 600 700 (nm) www.bipm.org 33 Vision and V() curve V(λ) filter www.bipm.org 3434 1979, new definition and introduction of Km Introduction of Km I [cd] diaphragm S P [W] φ d2 I = S d φ [lm] P [W] 380 480 580 680 780 Wavelength (nm) www.bipm.org 35 1979, new definition and introduction of Km Introduction of Km I [cd] diaphragm S P [W] φ d2 I = S d φ [lm] P [W] P ⋅ V() dλ φ 380 480 580 680 780 Wavelenght (nm) www.bipm.org 36 1979, new definition and introduction of Km Introduction of Km I [cd] diaphragm S P [W] φ d2 I = S d φ [lm] P [W] P ⋅ V() dλ φ = Km [lm⋅W‐1] 380 480 580 680 780 Wavelength (nm) www.bipm.org 37 1979, new definition and introduction of Km Definition of the candela I [cd] Km P S d λmax «The candela is the luminous intensity, in a given direction, of a source that emits monochromatic radiation of frequency 540 THz and that has a radiant intensity in that direction of 1/683 watt per steradian» 1979 : XVIème CGPM www.bipm.org 38 Success story : Photometry Standard Photopic observer (CIE 1924) Luminous efficiency ‐1 Kcd = 638 lm⋅W 0 Luminous intensity 555 Wavelenght (nm) (visual) SI brochure Principle governing photometry www.bipm.org 39 What is missing New agreed human visual response function (mesopic and 10°) www.bipm.org 40 What is missing Challenge (1/2) The measurand is not accessible by the measuring instrument Measurand Object www.bipm.org 41 What is missing Challenge (2/2) The measurand may vary from one observer to an other Elaine Moynihan Lisle Le pont japonais, Giverny Miraï Monet www.bipm.org 42 Measurement of perceptive quantities Current method Radiometry & spectrophotometry Psychophysic Measurand experiments (perceptive) Standard observer Perception Normalization P ⋅ V() dλ model activity www.bipm.org 43 Measurement of perceptive quantities Future method RadiometryImage based & spectrophotometry radiometry PsychophysicMachine Measurand experimentsLearning (perceptive) Perceptive scale IndividualStandard Object observer (physical) Physical scale (measurable) Perception Artificial Normalization intelligencemodels activity www.bipm.org 44 The laser www.bipm.org 45 Cryogenic Radiometer Evacuation port Liquid helium Apertures : tank 5 mm 6 mm 7.5 mm Laser beam Brewster angle window Thermal screen International agreement and consistency Accuracy to SI <~0.01 % 100 ppm ur100 Kind courtesy of Armin Sperling, Armin PTB Kind courtesy of Transformative technology Invented in 60s in the USSR and the US Nobel prize to Basov, Prokhorov, Townes Was recognized as an amazing discovery “from science fiction” Was thought to be a useless “science toy”: “a solution looking for problem” www.bipm.org 49 From laser to WEB 2.0 Broad-band data transmission is enabled by fiber-optical communication Laser is a key component Dramatic impact on modern society in the past decade www.bipm.org 50 Manipulating single photons www.bipm.org 51 Second Quantum Revolution Ultrafast, “smart” computers Quantum internet (absolute security) Custom-designed quantum materials Quantum sensors Quantum-logic based standards www.bipm.org 52 Light sources 50/50 beamsplitter Correlation functions A Photo‐ g(2)(0)=1 : random, no correlation, ex.
Load more

Recommended publications
  • Photopic and Scotopic – the “Eyes” Have It
    Photopic and Scotopic – The “eyes” have it Dick Erdmann GE Specification Engineer In the human eye the perceived brightness of illumination depends of color. It takes more energy in the blue or red portion of the color spectrum to create the same sensation of brightness as in the yellow-green region. When it comes to sensing light in the human eye there are two main light-sensing cells called rods and cones. If one took a tube and looked straight ahead through it so that it allowed the field of view to be restricted 2 degrees, light photons would fall on the part of the eye called the fovea that consists mainly of cones. The peripheral area surrounding the fovea consists of both rods and cones with the rods outnumbering the cones about 10:1. Cones have a peak response in the yellow-green region of about 555 nano-meters and rods have a peak response in the bluish-green area of about 505 nano-meters. Because both the rods and cones have been shown to have different sensitivities to colors they can be represented by two different sensitivity curves called Photopic Curves (representing the cone) and Scotopic Curves (representing the rod). Years ago it was thought that the cones were responsible for daytime vision and rods for nighttime vision. Because of this, light meters that measure lighting levels such as footcandles, lumens, lux, etc. are weighted to the cone activated part of the eye ignoring the effect of rod-activated vision. But according to a study by Dr. Sam Berman and Dr.
    [Show full text]
  • Transmission of Scotopic Signals from the Rod to Rod-Bipolar Cell in the Mammalian Retina
    Vision Research 44 (2004) 3269–3276 www.elsevier.com/locate/visres Transmission of scotopic signals from the rod to rod-bipolar cell in the mammalian retina W. Rowland Taylor a,*, Robert G. Smith b a Neurological Sciences Institute, Oregon Health and Sciences University––West Campus, 505 NW 185th Avenue, Beaverton, OR 97006, United States b Department of Neuroscience, University of Pennsylvania, Philadelphia, PA Received 15 June 2004; received in revised form 27 July 2004 Abstract Mammals can see at low scotopic light levels where only 1 rod in several thousand transduces a photon. The single photon signal is transmitted to the brain by the ganglion cell, which collects signals from more than 1000 rods to provide enough amplification. If the system were linear, such convergence would increase the neural noise enough to overwhelm the tiny rod signal. Recent studies provide evidence for a threshold nonlinearity in the rod to rod bipolar synapse, which removes much of the background neural noise. We argue that the height of the threshold should be 0.85 times the amplitude of the single photon signal, consistent with the saturation observed for the single photon signal. At this level, the rate of false positive events due to neural noise would be masked by the higher rate of dark thermal events. The evidence presented suggests that this synapse is optimized to transmit the single photon signal at low scotopic light levels. Ó 2004 Elsevier Ltd. All rights reserved. Keywords: Retina; Synaptic transmission; Single photon; Photoreceptor; Visual threshold; Scotopic vision 1. Introduction produced by single photons are carried by only a few neurons, whereas all the rods and postreceptoral Many mammals have evolved excellent night vision, neurons in the pool generate noise.
    [Show full text]
  • Comparative Visual Function in Predatory Fishes from the Indian River Lagoon Author(S): D
    Comparative Visual Function in Predatory Fishes from the Indian River Lagoon Author(s): D. Michelle McComb, Stephen M. Kajiura, Andrij Z. Horodysky, and Tamara M. Frank Source: Physiological and Biochemical Zoology, Vol. 86, No. 3 (May/June 2013), pp. 285-297 Published by: The University of Chicago Press Stable URL: http://www.jstor.org/stable/10.1086/670260 . Accessed: 16/07/2013 16:00 Your use of the JSTOR archive indicates your acceptance of the Terms & Conditions of Use, available at . http://www.jstor.org/page/info/about/policies/terms.jsp . JSTOR is a not-for-profit service that helps scholars, researchers, and students discover, use, and build upon a wide range of content in a trusted digital archive. We use information technology and tools to increase productivity and facilitate new forms of scholarship. For more information about JSTOR, please contact [email protected]. The University of Chicago Press is collaborating with JSTOR to digitize, preserve and extend access to Physiological and Biochemical Zoology. http://www.jstor.org This content downloaded from 152.3.102.242 on Tue, 16 Jul 2013 16:00:41 PM All use subject to JSTOR Terms and Conditions 285 Comparative Visual Function in Predatory Fishes from the Indian River Lagoon D. Michelle McComb1,* Introduction Stephen M. Kajiura2 Teleost fishes represent a speciose vertebrate lineage that ra- Andrij Z. Horodysky3 diated into distinct aquatic habitats that present unique diver- Tamara M. Frank4 gent light qualities (Jerlov 1968). Selective pressure on the pi- 1Harbor Branch Oceanographic Institute at Florida Atlantic scine eye has resulted in an extensive array of both 2 University, Fort Pierce, Florida 34946; Biological Sciences, morphological and physiological adaptations to maximize vi- Florida Atlantic University, Boca Raton, Florida 33431; sual function under differing light conditions.
    [Show full text]
  • Radiometric and Photometric Measurements with TAOS Photosensors Contributed by Todd Bishop March 12, 2007 Valid
    TAOS Inc. is now ams AG The technical content of this TAOS application note is still valid. Contact information: Headquarters: ams AG Tobelbaderstrasse 30 8141 Unterpremstaetten, Austria Tel: +43 (0) 3136 500 0 e-Mail: [email protected] Please visit our website at www.ams.com NUMBER 21 INTELLIGENT OPTO SENSOR DESIGNER’S NOTEBOOK Radiometric and Photometric Measurements with TAOS PhotoSensors contributed by Todd Bishop March 12, 2007 valid ABSTRACT Light Sensing applications use two measurement systems; Radiometric and Photometric. Radiometric measurements deal with light as a power level, while Photometric measurements deal with light as it is interpreted by the human eye. Both systems of measurement have units that are parallel to each other, but are useful for different applications. This paper will discuss the differencesstill and how they can be measured. AG RADIOMETRIC QUANTITIES Radiometry is the measurement of electromagnetic energy in the range of wavelengths between ~10nm and ~1mm. These regions are commonly called the ultraviolet, the visible and the infrared. Radiometry deals with light (radiant energy) in terms of optical power. Key quantities from a light detection point of view are radiant energy, radiant flux and irradiance. SI Radiometryams Units Quantity Symbol SI unit Abbr. Notes Radiant energy Q joule contentJ energy radiant energy per Radiant flux Φ watt W unit time watt per power incident on a Irradiance E square meter W·m−2 surface Energy is an SI derived unit measured in joules (J). The recommended symbol for energy is Q. Power (radiant flux) is another SI derived unit. It is the derivative of energy with respect to time, dQ/dt, and the unit is the watt (W).
    [Show full text]
  • Color Vision and Night Vision Chapter Dingcai Cao 10
    Retinal Diagnostics Section 2 For additional online content visit http://www.expertconsult.com Color Vision and Night Vision Chapter Dingcai Cao 10 OVERVIEW ROD AND CONE FUNCTIONS Day vision and night vision are two separate modes of visual Differences in the anatomy and physiology (see Chapters 4, perception and the visual system shifts from one mode to the Autofluorescence imaging, and 9, Diagnostic ophthalmic ultra- other based on ambient light levels. Each mode is primarily sound) of the rod and cone systems underlie different visual mediated by one of two photoreceptor classes in the retina, i.e., functions and modes of visual perception. The rod photorecep- cones and rods. In day vision, visual perception is primarily tors are responsible for our exquisite sensitivity to light, operat- cone-mediated and perceptions are chromatic. In other words, ing over a 108 (100 millionfold) range of illumination from near color vision is present in the light levels of daytime. In night total darkness to daylight. Cones operate over a 1011 range of vision, visual perception is rod-mediated and perceptions are illumination, from moonlit night light levels to light levels that principally achromatic. Under dim illuminations, there is no are so high they bleach virtually all photopigments in the cones. obvious color vision and visual perceptions are graded varia- Together the rods and cones function over a 1014 range of illu- tions of light and dark. Historically, color vision has been studied mination. Depending on the relative activity of rods and cones, as the salient feature of day vision and there has been emphasis a light level can be characterized as photopic (cones alone on analysis of cone activities in color vision.
    [Show full text]
  • Radiometry and Photometry
    Radiometry and Photometry Wei-Chih Wang Department of Power Mechanical Engineering National TsingHua University W. Wang Materials Covered • Radiometry - Radiant Flux - Radiant Intensity - Irradiance - Radiance • Photometry - luminous Flux - luminous Intensity - Illuminance - luminance Conversion from radiometric and photometric W. Wang Radiometry Radiometry is the detection and measurement of light waves in the optical portion of the electromagnetic spectrum which is further divided into ultraviolet, visible, and infrared light. Example of a typical radiometer 3 W. Wang Photometry All light measurement is considered radiometry with photometry being a special subset of radiometry weighted for a typical human eye response. Example of a typical photometer 4 W. Wang Human Eyes Figure shows a schematic illustration of the human eye (Encyclopedia Britannica, 1994). The inside of the eyeball is clad by the retina, which is the light-sensitive part of the eye. The illustration also shows the fovea, a cone-rich central region of the retina which affords the high acuteness of central vision. Figure also shows the cell structure of the retina including the light-sensitive rod cells and cone cells. Also shown are the ganglion cells and nerve fibers that transmit the visual information to the brain. Rod cells are more abundant and more light sensitive than cone cells. Rods are 5 sensitive over the entire visible spectrum. W. Wang There are three types of cone cells, namely cone cells sensitive in the red, green, and blue spectral range. The approximate spectral sensitivity functions of the rods and three types or cones are shown in the figure above 6 W. Wang Eye sensitivity function The conversion between radiometric and photometric units is provided by the luminous efficiency function or eye sensitivity function, V(λ).
    [Show full text]
  • The Eye and Night Vision
    Source: http://www.aoa.org/x5352.xml Print This Page The Eye and Night Vision (This article has been adapted from the excellent USAF Special Report, AL-SR-1992-0002, "Night Vision Manual for the Flight Surgeon", written by Robert E. Miller II, Col, USAF, (RET) and Thomas J. Tredici, Col, USAF, (RET)) THE EYE The basic structure of the eye is shown in Figure 1. The anterior portion of the eye is essentially a lens system, made up of the cornea and crystalline lens, whose primary purpose is to focus light onto the retina. The retina contains receptor cells, rods and cones, which, when stimulated by light, send signals to the brain. These signals are subsequently interpreted as vision. Most of the receptors are rods, which are found predominately in the periphery of the retina, whereas the cones are located mostly in the center and near periphery of the retina. Although there are approximately 17 rods for every cone, the cones, concentrated centrally, allow resolution of fine detail and color discrimination. The rods cannot distinguish colors and have poor resolution, but they have a much higher sensitivity to light than the cones. DAY VERSUS NIGHT VISION According to a widely held theory of vision, the rods are responsible for vision under very dim levels of illumination (scotopic vision) and the cones function at higher illumination levels (photopic vision). Photopic vision provides the capability for seeing color and resolving fine detail (20/20 of better), but it functions only in good illumination. Scotopic vision is of poorer quality; it is limited by reduced resolution ( 20/200 or less) and provides the ability to discriminate only between shades of black and white.
    [Show full text]
  • Artificial Eye for Scotopic Vision with Bioinspired All-Optical Photosensitivity Enhancer
    Artificial eye for scotopic vision with bioinspired all-optical photosensitivity enhancer Hewei Liua, Yinggang Huanga, and Hongrui Jianga,b,c,d,1 aDepartment of Electrical and Computer Engineering, University of Wisconsin-Madison, Madison, WI 53706; bMcPherson Eye Research Institute, University of Wisconsin-Madison, Madison, WI 53706; cDepartment of Materials Science and Engineering, University of Wisconsin-Madison, Madison, WI 53706; and dDepartment of Biomedical Engineering, University of Wisconsin-Madison, Madison, WI 53706 Edited by John A. Rogers, University of Illinois, Urbana, IL, and approved February 5, 2016 (received for review September 9, 2015) The ability to acquire images under low-light conditions is critical imaging systems, or combined with other image enhancement for many applications. However, to date, strategies toward improv- technologies. As an example, we present an artificial eye (Fig. 1 ing low-light imaging primarily focus on developing electronic image B and C) for scotopic vision using our all-optical photosensitivity sensors. Inspired by natural scotopic visual systems, we adopt an all- enhancer (Fig. 1D). Experimental results show the key aspects of optical method to significantly improve the overall photosensitivity optics and fabrication of the functional device. of imaging systems. Such optical approach is independent of, and Fig. 1E shows a 3D layout of the artificial eye and the structure can effectively circumvent the physical and material limitations of, of the bioinspired μ-PCs (Fig. 1E, Inset and SI Appendix, Fig. S2). the electronics imagers used. We demonstrate an artificial eye Our artificial eye (diameter R = 12.5 mm) consists of a ball lens inspired by superposition compound eyes and the retinal struc- (BK-7 glass, R = 6 mm) mounted in a central iris (R = 4 mm), ture of elephantnose fish.
    [Show full text]
  • Application Note
    How Light Meters Can Fool Us A primer on why bluer white light looks brighter to us and how it can help save the planet Imagine two identical rooms artificially illuminated with exactly the same amount of white light. A light meter confirms that the two rooms have equal light levels. In fact, everything about the rooms is the same except for one important detail: The light in one room has a little more blue in it than the other room. Why, then, does the room with the bluer light seem so much brighter? (See Fig. 1.) For decades this effect has created more than a little controversy among vision scientists, with many dismissing it as nothing more than an illusion. But recent advances in vision science now support the view that this is a real effect. The room with the bluer light does appear brighter to the human eye — a fact that can help reduce lighting costs by as much as 40% or more. To understand why, we need to know a little more about the history of why light meters are calibrated the way they are and how our eyes react to light. Figure 1: The shopping center above was initially lighted by fluorescent lamps having a color temperature of 4100K (left photo). The fluorescents were replaced by LEDs with a color temperature of 6000K (right photo). Even though the LED lamps use less electricity, the area still looks brighter because LED lighting is more efficient, but also because the higher color temperature creates a bluer white light that looks brighter to us.
    [Show full text]
  • Early Scotopic Dark Adaptation
    Early Scotopic Dark Adaptation A dissertation presented by Rebecca J. Grayhem To The Department of Psychology In partial fulfillment of the requirements for the degree of Doctor of Philosophy In the field of Psychology Northeastern University Boston, Massachusetts December, 2010 1 EARLY SCOTOPIC DARK ADAPTATION by Rebecca J. Grayhem ABSTRACT OF DISSERTATION Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Psychology in the Graduate School of Arts and Sciences of Northeastern University, December 2010 2 Abstract The human visual system can function over a broad range of light levels, from few photons to bright sunshine. I am interested in sensitivity regulation of the rod pathway in dim light, below the level at which the cones become effective. I obtained thresholds for large (1.3 deg) and tiny (5 min arc) circular test spots, either after 20-30 mins exposure to complete darkness (absolute threshold), or on uniform backgrounds of varying light intensities, or just after the background was removed to plunge the eye into darkness; Maxwellian view optics were used so that variations in pupil size would have no effect. The overall theory is that sensitivity in the rod system is adjusted by a slow process of adaptation in the retina driven by the long-term mean background light level and a rapid process sensitive to variability in the light provided by the background (“photon noise”). My data show that thresholds for tiny test spots primarily reveal the photon-driven noise effect, and those for large test spots reveal both processes. The traditional idea that all components of rod dark adaptation are slow is challenged here, since almost immediately after the background light is removed, thresholds of tiny spots drop to absolute threshold directly, and thresholds of large test spots drop half-way to absolute threshold before continuing to recover back to absolute threshold over the next 25 minutes.
    [Show full text]
  • Perception of Light in Virtual Reality
    Perception of Light in Virtual Reality DIPLOMARBEIT zur Erlangung des akademischen Grades Diplom-Ingenieurin im Rahmen des Studiums Visual Computing eingereicht von Laura R. Luidolt, BSc Matrikelnummer 01427250 an der Fakultät für Informatik der Technischen Universität Wien Betreuung: Associate Prof. Dipl.-Ing. Dipl.-Ing. Dr.techn. Michael Wimmer Mitwirkung: Univ.Ass. Dipl.-Ing. Katharina Krösl, BSc Wien, 2. Februar 2020 Laura R. Luidolt Michael Wimmer Technische Universität Wien A-1040 Wien Karlsplatz 13 Tel. +43-1-58801-0 www.tuwien.ac.at Perception of Light in Virtual Reality DIPLOMA THESIS submitted in partial fulfillment of the requirements for the degree of Diplom-Ingenieurin in Visual Computing by Laura R. Luidolt, BSc Registration Number 01427250 to the Faculty of Informatics at the TU Wien Advisor: Associate Prof. Dipl.-Ing. Dipl.-Ing. Dr.techn. Michael Wimmer Assistance: Univ.Ass. Dipl.-Ing. Katharina Krösl, BSc Vienna, 2nd February, 2020 Laura R. Luidolt Michael Wimmer Technische Universität Wien A-1040 Wien Karlsplatz 13 Tel. +43-1-58801-0 www.tuwien.ac.at Erklärung zur Verfassung der Arbeit Laura R. Luidolt, BSc Hiermit erkläre ich, dass ich diese Arbeit selbständig verfasst habe, dass ich die verwen- deten Quellen und Hilfsmittel vollständig angegeben habe und dass ich die Stellen der Arbeit – einschließlich Tabellen, Karten und Abbildungen –, die anderen Werken oder dem Internet im Wortlaut oder dem Sinn nach entnommen sind, auf jeden Fall unter Angabe der Quelle als Entlehnung kenntlich gemacht habe. Wien, 2. Februar 2020 Laura R. Luidolt v Acknowledgements First of all, I would like to thank Prof. Michael Wimmer for his guidance during this work.
    [Show full text]
  • Night Vision in the Elderly: Consequences for Seeing Through a ‘‘Blue Filtering’’ Intraocular Lens
    1518 PERSPECTIVE Br J Ophthalmol: first published as 10.1136/bjo.2005.073734 on 18 October 2005. Downloaded from Night vision in the elderly: consequences for seeing through a ‘‘blue filtering’’ intraocular lens J S Werner ............................................................................................................................... Br J Ophthalmol 2005;89:1518–1521. doi: 10.1136/bjo.2005.073734 Relative scotopic spectral sensitivity depends only on the spectral sensitivity maximum. Their analyses considered the percentage change in sensitivity. rhodopsin photopigment and ocular media absorption Here, we shall consider the same issue, but spectra. Rhodopsin is well characterised so the relative illustrated more traditionally in logarithmic units scotopic spectral sensitivity function can be calculated for so that the losses can be seen in the context of the full range of scotopic sensitivity. It will be intraocular lenses (IOLs) of known spectral density. In a shown why IOL absorption of light at wave- recent perspective, Mainster and Sparrow concluded that lengths near the sensitivity maximum is no more an IOL with short wave absorbing chromophores would important for scotopic vision than absorption at any other wavelengths. We shall also consider provide more retinal protection than conventional IOLs, but some aspects of scotopic vision not discussed by the practical consequences for scotopic vision are unclear. Mainster and Sparrow. In particular, the con- This paper uses published experiments to examine the sequences of IOL absorption spectra are evalu- ated in terms of scotopic spatial contrast implications for scotopic vision of the IOLs analysed by sensitivity as a quantitative index of pattern, or Mainster and Sparrow. A 14.6% reduction in scotopic form, vision. sensitivity is expected for a SN60AT (AcrySof Natural) compared to a SA60AT (Conventional AcrySof) IOL under SCOTOPIC SPECTRAL SENSITIVITY WITH AN IOL CONTAINING CHROMOPHORES broadband illumination (equal quantum spectrum).
    [Show full text]