Sept 16, 2005Ast 920 Meeting 21 Astronomy 920 Commissioning of the Prime Focus Imaging Spectrograph Meeting 2 Intro; VPH Grating Spectroscopy Ken Nordsieck.

Slides:



Advertisements
Similar presentations
Agenda Monday –Diffraction – Problems –How small? –How many? Tuesday –Diffraction – Laboratory, Quiz on Interference Wed –Review Fri –Bonus Quiz.
Advertisements

SALT RSS-NIR MID-TERM REVIEW MAY 20 & 21, 2009 ANALYTIC OPTICS KENNETH NORDSIECK UNIVERSITY OF WISCONSIN.
The waves spread out from the opening!
Instead of shining monochromatic light (e.g. a laser) through a diffraction grating, what would happen if we shone a polychromatic light source (e.g. white.
Spectroscopic Data ASTR 3010 Lecture 16 Textbook Ch. 11.
Double Slit Diffraction Physics 202 Professor Lee Carkner Lecture 27.
Lecture 33 Review for Exam 4 Interference, Diffraction Reflection, Refraction.
Prismswww.edmundoptics.com Right AngleEquilateralPentagonalDove.
Interference and Diffraction
Double Slit Diffraction Physics 202 Professor Lee Carkner Lecture 27.
Interference and Diffraction
PHY 1371Dr. Jie Zou1 Chapter 38 Diffraction and Polarization (Cont.)
© 2012 Pearson Education, Inc. { Chapter 36 Diffraction (cont.)
Diffraction Applications Physics 202 Professor Lee Carkner Lecture 28.
Spectrographs. Spectral Resolution d 1 2 Consider two monochromatic beams They will just be resolved when they have a wavelength separation of d Resolving.
Astronomical Spectroscopy
Oct 17, 2001SALT PFIS PDR - Structure1 Structure Interface/ constraints Loads Structure design rationale Truss Weight and CG Finite Element Analysis/ Image.
VOLUME-PHASE HOLOGRAPHIC GRATINGS FOR ASTRONOMICAL SPECTROGRAPHS James A. Arns, Willis S. Colburn, & Mark Benson (Kaiser Optical Systems, Inc.) Samuel.
Astronomical Instrumentation Often, astronomers use additional optics between the telescope optics and their detectors. This is called the instrumentation.
THE LHIRES-III SPECTROGRAPH © C2PU, Observatoire de la Cote d’Azur, Université de Nice Sophia-Antipolis Jean-Pierre Rivet CNRS, OCA, Dept. Lagrange
Instrumentation Concepts Ground-based Optical Telescopes Keith Taylor (IAG/USP) ‏ Aug-Nov, 2008 Aug-Sep, 2008 IAG-USP (Keith Taylor)‏
Spectrographs. Literature: Astronomical Optics, Daniel Schneider Astronomical Observations, Gordon Walker Stellar Photospheres, David Gray.
Daily Challenge, 1/7 If light is made of waves and experiences interference, how will the constructive and destructive interference appear to us?
Spectroscopy principles
14 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
High Resolution Echelle Spectrograph for Chinese Weihai 1m Telescope. Leiwang, Yongtian Zhu, Zhongwen Hu Nanjing institute of Astronomical Optics Technology.
18 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
Astronomical Spectroscopy Notes from Richard Gray, Appalachian State, and D. J. Schroeder 1974 in “Methods of Experimental Physics, Vol. 12-Part A Optical.
Multiplexed High Res Spectroscopy at Keck – J. Cohen (PI), H. Epps (Optical Design), M. Rich (Project Scientist) Keck instruments for optical spectroscopy.
JGR 19 Apr Basics of Spectroscopy Gordon Robertson (University of Sydney)
Waves: Diffraction Gratings
NEXT GENERATION OPTICAL SPECTROGRAPH FOR NOAO Samuel Barden, Charles Harmer, Taft Armandroff, Arjun Dey, and Buell Jannuzi (National Optical Astronomy.
Oct 30, 2003PFIS - Student Wkshop1 The Prime Focus Imaging Spectrograph – Old Challenges and New Ones K. Nordsieck, Principal Investigator Jeff Percival,
Chapter 16 Pretest Interference and Diffraction. 1. When monochromatic light is reflected from a thin transparent film, A) constructive interference occurs.
Dr. Quantum General Physics 2Light as a Wave1. General Physics 2Light as a Wave2 The Nature of Light When studying geometric optics, we used a ray model.
The waves spread out from the opening!
The Prime Focus Imaging Spectrograph Design and Capabilities
Oct 26, 2007SALT Workshop UKZN1 Robert Stobie Prime Focus Imaging Spectrograph Science Rationale Modes –Fabry-Perot Spectral Imaging –Grating Spectroscopy;
Interference & Diffraction Gratings
Lab 10: Wave optics Only 2 more labs to go!! Light is an electromagnetic wave. Because of the wave nature of light it interacts differently than you might.
Instrumentation Concepts Ground-based Optical Telescopes Keith Taylor (IAG/USP) ‏ Aug-Nov, 2008 Aug-Sep, 2008 IAG-USP (Keith Taylor)‏
Oct 17, 2001SALT PFIS PDR - Optics1 Optics Refractive Optics - Design rationale Performance Slitmasks Gratings Polarimetric Optics Risks and Concerns Kenneth.
Goals for HETDEX Determine equation of state of Universe and evolutionary history for dark energy from 0
Laser Spectroscopy/SJX Chap. 4 Components of Spectroscopic Instruments 1 In this chapter we discuss basic spectroscopic instruments and techniques employed.
F. Pepe Observatoire de Genève Optical astronomical spectroscopy at the VLT (Part 2)
Optical astronomical spectroscopy at the VLT (Part 1) F. Pepe Observatoire de Genève.
The Prime Focus Imaging Spectrograph for the Southern African Large Telescope: Operational Modes Chip Kobulnicky – Instrument Scientist, University of.
2. Diffraction Grating Basic principles: Diffraction
Overview: Astronomical Spectroscopy Basic Spectrograph Optics Objective Prism Spectrographs Slit Spectrographs.
Prime Focus Imaging Spectrograph Status
Diffraction Gratings.
Astronomy 920 Commissioning of the Prime Focus Imaging Spectrograph
Wave Phenomena Resolution
THE LHIRES-III SPECTROGRAPH
Astronomy 920 Commissioning of the Prime Focus Imaging Spectrograph
Astronomy 920 Commissioning of the Prime Focus Imaging Spectrograph
Introduction to Spectroscopy
Meeting 10 Longslit Spectroscopy Ken Nordsieck
Example: 633 nm laser light is passed through a narrow slit and a diffraction pattern is observed on a screen 6.0 m away. The distance on the screen.
Overview Instrument Role Science Niches Consortium science
Polarimetry: Waveplate Modulation; Calibration
Diffraction Grating.
The scattering centre becomes a secondary source of radiation
The Geometry of Interference and Diffraction
BASIC HYPER SPECTRAL IMAGING
Meeting 11 Polarimetry: Beamsplitter; data formats Ken Nordsieck
Key areas The relationship between the wavelength, distance between the sources, distance from the sources and the spacing between maxima or minima. The.
The waves spread out from the opening!
Meeting 9 Slitmask Planning Ken Nordsieck
PFIS Commissioning - SSII
Presentation transcript:

Sept 16, 2005Ast 920 Meeting 21 Astronomy 920 Commissioning of the Prime Focus Imaging Spectrograph Meeting 2 Intro; VPH Grating Spectroscopy Ken Nordsieck

Sept 16, 2005Ast 920 Meeting 22 Optics Layout

Sept 16, 2005Ast 920 Meeting 23 VPH Gratings

Sept 16, 2005Ast 920 Meeting 24 Throughput

Sept 16, 2005Ast 920 Meeting 25 NIR Upgrade Path NIR upgrade path preserved by collimator allowing full 320 nm – 1.7 μ wavelength range + support structure

Sept 16, 2005Ast 920 Meeting 26 Assembly and Integration

Sept 16, 2005Ast 920 Meeting 27 Slitmask Cutter Commercial laser MOS: custom slits cut in carbon-fiber Longslit: stainless steel, tilted and polished for viewing by SALTICAM/ slitviewer optics PI planning tool produces slitmask file for inclusion in proposal

Sept 16, 2005Ast 920 Meeting 28 Grating Optics Grating Equation Resolution Why Large Telescope Spectrographs are Big VPH Gratings

Sept 16, 2005Ast 920 Meeting 29 Grating Equation and Resolution m λ / Λ = sin α + sin β = 2 sin α (Littrow) dλ / dβ = (Λ/m) cos β angular size of monochromatic slit: Δα = Δθ D tel / D col Δβ = Δα cos α / cos β Δλ (slit) = (Λ/m) cos α Δθ D tel / D col at Littrow R = λ/Δλ (slit) = 2 (D col / D tel ) tan α / Δθ D tel = dia of primary D col = dia of collimated beam Λ = spacing of grating grooves θ = angle in sky α = angle of incidence β = angle of diffraction m = order of diffraction

Sept 16, 2005Ast 920 Meeting 210 Resolution R = λ/Δλ (slit) = 2 (D col / D tel ) tan α / Δθ Does *not* depend on –diffraction order (!) –grating groove density (!) For fixed seeing, improve only by –going to higher grating angle (eg Echelle) –increasing the size of your collimated beam ($$) Note: for small telescopes, also worry about grating diffraction limit R dif = D grat /Λ For SALT/ PFIS: D col = 150 mm, D tel / D col = 73.3 R = 5640 for 1 arcsec slit, 45 deg grating angle

Sept 16, 2005Ast 920 Meeting 211 VPH Gratings Created by exposing holograph material (“DCG”) to interference pattern from laser Index of refraction of DCG is modulated in space Large; inexpensive; custom design; efficient at high groove density

Sept 16, 2005Ast 920 Meeting 212 PFIS VPH 1300 gr/ mm VPH (Λ = 769 nm)

Sept 16, 2005Ast 920 Meeting 213 Tunable “Blaze” Peak efficiency is at Littrow => “Blaze angle” changes with α If increase β as tilt grating, can use grating at large range of central wavelengths => change camera angle = α + β