 Myth: 3 sec memory  Reality: 3 years are passed  I’m not a goldfish, but…

Slides:



Advertisements
Similar presentations
1 ATST Imager and Slit Viewer Optics Ming Liang. 2 Optical layout of the telescope, relay optics, beam reducer and imager. Optical Layouts.
Advertisements

 Normal Standard Model  Fast telescope  New coatings  CCD Window Ghost  Ghost simulator Catania,28-2,01-03 Matteo Munari – INAF OACt.
Interference and Diffraction
WHY STUDY ASTROPHYSICS?  To gain an understanding of our universe and our role in it Learn about how the universe operates --> modern science  Observations.
Blizard Advanced Light Microscopy club Making friends with your microscope.
Atmospheric Effects and Other Observational Issues AS3100 Lab. Astronomi Dasar 1 Prodi Astronomi 2007/2008 B. Dermawan.
Chapter 15 Pretest Light and Refraction
Unit 33 - Optics Optics is the study of the behavior and properties of light. This includes it’s interactions with objects including mirrors, lenses, and.
Image reconstruction and analysis for X-ray computed microtomography Lucia Mancini 1, Francesco Montanari 2, Diego Dreossi 3 1 Elettra - Trieste 2 A.R.P.A.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
Chapters 28 Reflection and Refraction. Topics Reflection Law of Reflection – plane mirrors – diffuse reflection Refraction – Mirage Cause of Refraction.
Demetrio Magrin INAF – Astronomical Observatory of Padova Optical Design Catania, 11/06/2014.
PACS IIDR 01/02 Mar 2001 Baffle and Straylight1 D. Kampf KAYSER-THREDE.
Camera/Video. CCD DSP lux 3.6 mm f/ deg. 1/3”
 Mirrors that are not flat are called curved mirrors.  Depending on whether the reflective coating is on the inside or outside of the curve will decide.
1 UCT PHY1025F: Geometric Optics Physics 1025F Geometric Optics Dr. Steve Peterson OPTICS.
P3 Physics Revision checklist Optics, Lenses and the Eye (1)
Echelle spectra reduction with IRAF*
Many sources (hot, glowing, solid, liquid or high pressure gas) show a continuous spectra across wavebands. Emission spectra Elements in hot gases or.
Chapter 23 Mirrors and Lenses.
Light: Geometric Optics
Deep Impact Projectsmfa - 1 Deep Impact Projects (2) Mike A’Hearn.
SECCI/COR2 Status Report SECCHI CONSORTIUM MEETING D. Socker, S. Plunkett, A. Vourlidas.
Telescopes (Chapter 6). Based on Chapter 6 This material will be useful for understanding Chapters 7 and 10 on “Our planetary system” and “Jovian planet.
Copyright © 2009 Pearson Education, Inc. Chapter 32 Light: Reflection and Refraction.
Light and Telescopes Chapter 5. Radio Interferometry The Very Large Array (VLA): 27 dishes are combined to simulate a large dish of 36 km in diameter.
IRMS Optical Subsystem Review. The Charter Confirm that the MOSFIRE design is a feasible baseline for IRMS (yes) Verify that the MOSFIRE design can achieve.
J.P. Halain – Centre Spatial de Liège
Physics 1051 Lecture 7 Slide 1 Refraction of Light –Part 2.
We see things because they _____________ light into our eyes.
E-  identification 1. Reminder from previous presentations, questions, remarks 2. Čerenkov option 3. Study of several optical configurations 4. Conclusions.
PHY2049 Summer 2011 The following clicker numbers are no longer going to be counted. They have not been registered Exam.
TELESCOPES. WHAT IS A TELESCOPE A telescope is an instrument that gathers electromagnetic radiation from objection in space and concentrates it for better.
1 Optics Electromagnetic spectrum polarization Laws of reflection and refraction TIR –Images –Mirrors and lenses –Real/virtual, inverted/straight, bigger/smaller.
REFRACTION. When light travels from one material to another it usually changes direction The bending of light that occurs at the borderline of two materials.
A photon checks into a hotel. The desk clerk asks, “Do you need help with your luggage?” The photon replies, “I don’t have any. I’m travelling light.”
Eusoballoon optics characterisation Camille Catalano and the Toulouse team Test configuration Calibration of the beam Exploration of the focal plan.
Optical characteristics of the EUV spectrometer for the normal-incidence region L. Poletto, G. Tondello Istituto Nazionale per la Fisica della Materia.
ECEN 4616/5616 Optoelectronic Design Class website with past lectures, various files, and assignments: (The.
1 Components of Optical Instruments, Cont… Lecture 7.
Dennis C. Evans p1 SuperNova/Acceleration Probe 16 November 2001 Optical Analysis & Stray Light Evaluation Optical Analysis and Stray Light Evaluation.
1 Chapter 34 One of the most important uses of the basic laws governing light is the production of images. Images are critical to a variety of fields and.
Naoyuki Tamura (University of Durham) Expected Performance of FMOS ~ Estimation with Spectrum Simulator ~ Introduction of simulators  Examples of calculations.
Visual Angle How large an object appears, and how much detail we can see on it, depends on the size of the image it makes on the retina. This, in turns,
Basic Astronomy Basics about telescope and how to view the cosmos.
Unit One: Matter and Energy Flow in Cells
Integral Field Spectrograph Eric PRIETO CNRS,INSU,France,Project Manager 11 November 2003.
15 October Observational Astronomy Direct imaging Photometry Kitchin pp ,
Geometric Optics. An object inside the focus casts a virtual image that is only focused by the eye.
1. How is the index of refraction calculated? How is light refracted as it speeds up? How is light refracted as it slows down? Index of refraction = speed.
September 16, 2008LSST Camera F2F1 Camera Calibration Optical Configurations and Calculations Keith Bechtol Andy Scacco Allesandro Sonnenfeld.
1 Perception and VR MONT 104S, Fall 2008 Lecture 21 More Graphics for VR.
READING: Units: 59, 60. The Family of Stars Stars come in all sizes…
3M Touch Systems © 3M All Rights Reserved 3M CONFIDENTIAL Touch Screen Optics Training.
14 Sep 2000ASTR103, GMU, Dr. Correll1 ASTR 103--Week 3.
Light. Photon is a bundle of light related to the amount of energy Light travels in straight line paths called light rays
Refraction of Light –Part 2. Internal Reflection When light travels from a slow medium to a fast medium, the angle of refraction is larger than the angle.
14FEB2005/KWCAE2-UsersGroup Astro-E2 X-Ray Telescopes XRT Setup & Structure Performance Characteristics –Effective Area –Angular Resolution –Optical Axes.
UNIT 1: WAVES Lesson 2 Introduction: Light. Remember… Light waves do not need a medium to travel through. What are the type of waves called that do not.
Mirror and Reflection.
Chapter 24: Perception April 20, Introduction Emphasis on vision Feature extraction approach Model-based approach –S stimulus –W world –f,
PACS IIDR 01/02 Mar 2001 Optical System Design1 N. Geis MPE.
Today’s agenda: Plane Mirrors. You must be able to draw ray diagrams for plane mirrors, and be able to calculate image and object heights, distances, and.
Color  You see an object as the wavelength  ( color) of visible light that it reflects  Sunflowers are yellow because it reflects (bounces off) mostly.
Optics: Reflection, Refraction Mirrors and Lenses
TOU Team PLATO Consortium Campi Bisenzio, 12 Dec 2016.
Point Source Transmission Simulations on the COROT baffle
Chapter 5 Telescopes.
Optics Investigate the properties and behaviors of mechanical and electromagnetic waves. Explore and explain the nature of sound and light energy.
Observational Astronomy
Presentation transcript:

 Myth: 3 sec memory  Reality: 3 years are passed  I’m not a goldfish, but…

 From PLATO-CAMTO-TS-90-LESIA  Dimension ed energy of Ghosts ▪ Extended and pointlike  Absent: requirements on scattered straylight ▪ Once there was a requirement: 20ph/pxl/s, but has been excluded (or forgot…), or my copy of the doc… ▪ Reduce to a PST/rejection requirement?  Requirements on transmission (to limit ‘blue’ light)  Requirements on cleanliness levels (not justified)

 It is the model of reference ZEMAX  Based on a slightly old design (some radii of curvature)  Structure is semiconceptual (tube & diaphgrams) 90% absorbing, 10% lambertian scattering  All lenses and window (front face included) have 1% AR coating  20A microroughness and CL500 dust on window  The CCD has a 1-QE reflectivity  Fed by a 240mm diam circular collimated source of 4W (1W on the entrance pupil), moved along the diagonal of FoV  Wavelength weighted to reproduce energy of a G0

 TOU-OPT28: Should a ghost image be focused on the detector, its relative intensity shall be less than 0.2% (TBC) of the flux of the star which creates the ghost.  Due to the presence the flat window  Using Rlenses=1%, Rccd=1-QE Deltam~6

 TOU-OPT27: The surface of ghost light beams at the detector surface shall be greater than 3000 pixels (TBC) Column Min

Up to mNstarsUp to mNstarsUp to mNstarsUp to mNstars E E E E E E E E E E E E E E E+08 Based on Allen (1973) m<10 Bahcall&Soneira m>10 Spectrum: G0 Number of stars in Plato TOU field up to the m mag

 Build a Ghost Simulator form several (105) zemax files and IDL routines.  Used in two ways  Single source: to extract data of ghosts: positions, radius and percentage of rays entering the pupil that can form the ghost  Multi source: using the previous stellar model, to simulate an entire field

MagStar Extended Ghosts Point-like ghosts Average due to extended ghostsVariance E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E E-04 TOTAL3.96E E E E-01 Brightes features are present from the beginning Adding higher mags adds an offset Evolution of extended ghosts with mag

Inside FoV is 2-2.5% (was 1% without CCD reflection) Outside FoV is similar to old 6 lenses or better because the tube is larger and exactly the same of that of ‘6 lenses’ Stars + Zodiacal light

 3 ‘families’ and 5 models  1-4,2-3 (N), 5(F)  Composed by two part  interface ring: ▪ identical for all models, ▪ is the interface with the TOU tube ▪ ‘hosts’ the window  Cone: ▪ different cut angle and height according to family ▪ Different orientations according to model TypeCut Angle Rotation angle H N exemplars (92)? (92)?

 Not for “direct” stray light from astronomical objects (they are too small)  Thermal?  On a ‘prudence basis’ to ‘fight’ TOU mutual scattering and satellite (sunshield) scattering  At the moment we don’t have any simulation to support that ▪ Simulations are difficult because ▪ We need information about all the system (disposition of TOUs, materials, sunshield…) ▪ The system is big but the single TOU pupil is small: raytracing may have poor statistic

 Requirements (from system?)  Model  Migration to ASAP  Optical design  Mechanical design  Coatings  Sources  Check calculations ph/s/pxl  Earth /Moon  Satellite / Mutual scattering