Commissioning. TripleSpec Design Review December 6-7, 2005 Update: March 12, 2008
|
|
- Lorraine Cummings
- 7 years ago
- Views:
Transcription
1 1 Commissioning Commissioning schedule overview Readiness to ship criteria Shipping and setup plan Daytime commissioning prior to observation On-sky evaluation of instrument performance Telescope time requirements summary
2 2 Commissioning Schedule Preparation Computer configuration testing ( T - 1 month) All instrument functionality in place with instrument specific flexible GUI's. Integration with TUI in progress. Instrument delivery ( T - 2 weeks) T 7 days in practice (instrument should pull up on Friday) Instrument team arrival ( T 5 days) Wilson (T - 8 days); Nelson/Skrutskie (T 3 days) Daytime testing of instrument on/off telescope ( T - 3 days) At APO discretion Observations (5 consecutive half nights allocated for first run; Two more engr runs scheduled) Two half-nights of evening engineering Day off / reserve half-night for evaluation Three full nights of engineering / commissioning science Dark time break (3 weeks) Four half nights for final commissioning
3 3 Readiness for Commissioning In order to be considered ready for shipping the following criteria must be met: Overall system No detectable warm leaks with helium leak checker. (Evaluate post cooldown pressure to assure no evidence for cold vacuum leaks.) Not quite. We lost access to the robust helium leak checker. The system was checked early on. Pumpdown and vacuum performance are the same as then. Cryogenic hold time > 36 hours. Measured at > 96 hours. All electronics and telemetry operating nominally, fully cabled and mounted in operating configuration. Instrument fully integrated with instrument cart. Both of the above items have been met. Alignment stable for at least three thermal cycles. Four UVa cooldowns with detectors. Spectrograph and slit viewer focus change between #2 and #3. Spectrograph and slit viewer stable between #1-2 and #3-4. Focus change as predicted by models.
4 4 Readiness for Commissioning In order to be considered ready for shipping the following criteria must be met: Slit Viewer channel Read noise <30 electrons in CDS (likely met) Dark current <100 electrons/s (weak requirement due to Ks background expect < 1 e-/sec) (likely met) Image degradation due to de-focus/tilt < 1 pixel (0.25 ) across array referenced to slit (ensquared energy criterion - >80% in a 4x4 pixel box) (TBD at telescope; confidence from reimage fiber end with <2 pixel FWHM) Throughput, including array quantum efficiency, >30% (TBD; thermal background levels as expected) Pupil location consistent with <5% misalignment at secondary mirror (met) Slit image motion due to axial rotation flexure < 100 um at array (met)
5 5 Readiness for Commissioning In order to be considered ready for shipping the following criteria must be met: Spectrograph channel Read noise < 15 electrons for CDS ( <16 e- Fowler 1; <5 e- Fowler16) Dark current < 0.1 electrons/second (measured at 0.15 e-/s at sea level, expect 2x lower on mountain) HAWAII-2 temperature stabilized to +/- 0.1K (maybe? not sure there is a significant requirement here; currently stabilized to auxiliary tank LN2 bath through significant heat strapping) Monochromatic slit image degraded by no more than 0.5 pixel at any position between 0.9 and 2.3 micron need to develop an appropriate ensquared energy spec. (focus analysis shows consistent 2 pixel psf across array; expected aberrations at edges/corners degrade to 3 pixels) Measured throughput exceeds 15% between 1.2 and 2.3 um (working on it... relative response looks identical to Cornell, stars will be the best arbiter.) Scattered light and ghosting from thermal background does not degrade background limited performance (along with no egregious ghosts from bright targets) (no problem)
6 6 Pre-ship Computer Testing This was just not feasible given the manpower commitment to the hardware. Prior to the shipment of the instrument to APO we will install and test the computer interfaces on site. This exercise will occur at least one month prior to instrument delivery at APO. Simulators will produce a data stream comparable to the output of both the slit-viewer and science-array channels. The exact timing of this exercise will be chosen to have minimum impact on the laboratory testing and commissioning of the main instrument (but may lead to a week of downtime for lab end-to-end testing).
7 7 Shipping Given authorization, the instrument and cart will be driven to APO by UVa staff no less than two weeks prior to its first night of operation. The instrument will be cooled immediately upon arrival and checked for functionality and stable alignment. The instrument will be left ready for observation. The full commissioning team will arrive 5 days before the first scheduled observations for final configuration and off-telescope / daytime testing.
8 8 Daytime Testing Both at the initial observatory cooldown and immediately before the observing run: Evaluate functionality and noise performance of the two imaging systems. Check alignments with telescope analog and monochromator Test system off (and possibly on) telescope Room lights and daylight sky with the mirror covers closed will provide useful calibration and test data. The pupil location relative to the secondary will be mapped (although this should not be necessary give lab alignment) Collect dome flats, dark frames, calibration lamp frames,...
9 9 Daytime Testing Astronomical observations to test the slit viewer channel can be conducted in daylight or bright twilight. Preliminary instrument blocks can be constructed in early twilight (as was done for CorMASS). Overall, the daytime/lab observations should largely validate the system for science readiness and efficient use of the allocated engineering commissioning night time.
10 10 On-sky Testing Chronology Validation of secondary illumination (1.5 hours) Target: any 6 th magnitude star The re-imager Lyot stop is shared by the slit-viewer and the spectrograph. Out-of-focus images on the slit-viewer will validate the alignment of the Lyot stop on the center of the secondary. A weak double-check can be made by looking at spectra of de-focused sources. Turning the rotator will confirm axial alignment of the emerging beam. Tolerance: Lyot boresight <5% off from center of secondary Illumination variation with rotation will not compromise photometry at >2% level
11 11 On-sky Testing Chronology Bright star spectrum (10 minutes) A first-light indulgence, while a bright star is handy. Ideally an A0 star for spectral throughput (Cornell is standing by to evaluate) Instrument block definition (1.5 hours) The slit viewer will provide real-time (frame-persecond) feedback for constructing an instrument block (a procedure which worked efficiently with the CorMASS slit viewer). With a 4 arcminute field initial source acquisition should be straightforward (it wasn t too difficult even with the 13 arcsec field of CorMASS) UVa must provide a utility for rapid (x,y) centroiding on the HAWAII-1 array
12 12 On-sky Testing Chronology Slit viewer characterization (1 hour) Star cluster Check slit image position vs. rotator position (daytime) Validate image quality and measure distortion across field (star field or cluster). Evaluate sensitivity using 2MASS photometry collect data to document limiting magnitude for guiding vs. integration time (can be done in parallel with spectroscopic observations throughout the night). Measure Ks-band system emissivity Evaluate interaction between bright stars and slit (slit edge effects, scattered light...)
13 13 On-sky Testing Chronology Basic spectrograph characterization (4 hours) Target spectral type A0 and G2 standards (magnitude 7-9) for primary quantitative continuum tests and bright planetary nebulae (NGC 7027) for emission line characterization. Collect data to evaluate the fundamentals HAWAII-2 focus and tilt slit response function along and across slit system throughput as a function of wavelength on-sky wavelength calibration
14 14 On-sky Testing Chronology Basic spectrograph characterization (continued) Target magnitude white dwarfs to evaluate ultimate system sensitivity for long integrations. establish background limited integration times in spectral regions between airglow lines as a function of wavelength. Observe at least one science rich target (e.g. NGC1068) which highlights both spectroscopic resolution and long slit capability.
15 15 Observing time requirements The on-sky tests in the previous slide will occupy the better part of two half nights. ideally these will be the first half so that the team can focus on data analysis in a well-rested state the subsequent morning/afternoon. A third contingency half night should be available with the expectation that it will be allocated to an ARC science program on another instrument if sufficient data have been collected to that point. TripleSpec staff will use the break for data analysis.
16 16 Observing time requirements A three full-night science run will follow presuming the instrument is in acceptable condition. As with the first CorMASS commissioning run we will observe a mix of targets those of interest to the instrument team as well as those requested by the ARC community. Raw data will be accessible to all (as well as the adapted SpexTool algorithms).
17 17 Observing time requirements We will address remaining software/hardware configuration issues during the dark-time period and return for four half-nights of final engineering/science toward the end of the next bright time period. The instrument will be ready for general use following this second observing run.
MY FIRST STEPS IN SLIT SPECTROSCOPY
MY FIRST STEPS IN SLIT SPECTROSCOPY Andrew Wilson BAAVSS Spectroscopy Workshop Norman Lockyer Observatory October 2015 Overview My choice of spectrograph, camera and telescope Getting started and basic
More informationFig.1. The DAWN spacecraft
Introduction Optical calibration of the DAWN framing cameras G. Abraham,G. Kovacs, B. Nagy Department of Mechatronics, Optics and Engineering Informatics Budapest University of Technology and Economics
More informationDevelopment of the Extreme Ultraviolet Spectrometer: EXCEED
Development of the Extreme Ultraviolet Spectrometer: EXCEED Go Murakami*, Kazuo Yoshioka, Atsushi Yamazaki, Tomoki Kimura Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency
More informationAlpy guiding User Guide. Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com)
Alpy guiding User Guide Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com) DC0017A : april 2013 Alpy guiding module User Guide Olivier Thizy (olivier.thizy@shelyak.com)
More informationCOOKBOOK. for. Aristarchos Transient Spectrometer (ATS)
NATIONAL OBSERVATORY OF ATHENS Institute for Astronomy, Astrophysics, Space Applications and Remote Sensing HELMOS OBSERVATORY COOKBOOK for Aristarchos Transient Spectrometer (ATS) P. Boumis, J. Meaburn,
More informationChapter 6 Telescopes: Portals of Discovery. How does your eye form an image? Refraction. Example: Refraction at Sunset.
Chapter 6 Telescopes: Portals of Discovery 6.1 Eyes and Cameras: Everyday Light Sensors Our goals for learning:! How does your eye form an image?! How do we record images? How does your eye form an image?
More informationScience Standard 4 Earth in Space Grade Level Expectations
Science Standard 4 Earth in Space Grade Level Expectations Science Standard 4 Earth in Space Our Solar System is a collection of gravitationally interacting bodies that include Earth and the Moon. Universal
More informationHigh Resolution Imaging in the Visible from the Ground without Adaptive Optics: New Techniques and Results
High Resolution Imaging in the Visible from the Ground without Adaptive Optics: New Techniques and Results Craig Mackay *a, John Baldwin b, Nicholas Law a and Peter Warner b a Institute of Astronomy and
More informationCryogenic Performance of Millitech Model FBI-22 Waveguide Isolator.
THE AUSTRALIA TELESCOPE NATIONAL FACILITY AT Technical Document Series AT/39.3/127 May 2, 2006 Cryogenic Performance of Millitech Model FBI-22 Waveguide Isolator. Russell Bolton Russell Gough Two model
More informationIntroduction to CCDs and CCD Data Calibration
Introduction to CCDs and CCD Data Calibration Dr. William Welsh San Diego State University CCD: charge coupled devices integrated circuit silicon chips that can record optical (and X-ray) light pixel =
More informationTHE BOHR QUANTUM MODEL
THE BOHR QUANTUM MODEL INTRODUCTION When light from a low-pressure gas is subject to an electric discharge, a discrete line spectrum is emitted. When light from such a low-pressure gas is examined with
More informationA STEP 400 Technical development status
A STEP 400 Technical development status ARENA workshop, Catania, 17 sept 08 Authors: J.B. Daban (1), C. Gouvret (1), A. Agabi (1), T. Guillot (2), F. Fressin (2), L. Abe (1), N. Crouzet (2), Y. Fanteï-Caujolle
More informationAssessments of LEDs IESNA LM-79, LM-80 & LM-82
Assessments of LEDs IESNA LM-79, LM-80 & LM-82 by Rolf S. Bergman Consultant 4/30/2012 1 ALA M Outline of Presentation Background Information EPA Energy Star specifications NVLAP Accreditation IESNA Technical
More informationMeasuring the Doppler Shift of a Kepler Star with a Planet
Measuring the Doppler Shift of a Kepler Star with a Planet 1 Introduction The Doppler shift of a spectrum reveals the line of sight component of the velocity vector ( radial velocity ) of the object. Doppler
More informationWe bring quality to light. MAS 40 Mini-Array Spectrometer. light measurement
MAS 40 Mini-Array Spectrometer light measurement Features at a glance Cost-effective and robust CCD spectrometer technology Standard USB interface Compatible with all Instrument Systems measuring adapters
More informationA remote diagnostics system for the MERLIN array. D. Kettle, N.Roddis Jodrell Bank Observatory University of Manchester Macclesfield SK11 9DL
A remote diagnostics system for the MERLIN array D. Kettle, N.Roddis Jodrell Bank Observatory University of Manchester Macclesfield SK11 9DL 1. Introduction Jodrell Bank Observatory operates an array of
More informationExtraction Heights for STIS Echelle Spectra
Instrument Science Report STIS 98-09 Extraction Heights for STIS Echelle Spectra Claus Leitherer and Ralph Bohlin March 1998 ABSTRACT The optimum extraction height (h) for STIS echelle spectra of 7 pixels
More informationDetecting and measuring faint point sources with a CCD
Detecting and measuring faint point sources with a CCD Herbert Raab a,b a Astronomical ociety of Linz, ternwarteweg 5, A-400 Linz, Austria b Herbert Raab, chönbergstr. 3/1, A-400 Linz, Austria; herbert.raab@utanet.at
More informationRESULTS FROM A SIMPLE INFRARED CLOUD DETECTOR
RESULTS FROM A SIMPLE INFRARED CLOUD DETECTOR A. Maghrabi 1 and R. Clay 2 1 Institute of Astronomical and Geophysical Research, King Abdulaziz City For Science and Technology, P.O. Box 6086 Riyadh 11442,
More informationHow to buy a telescope for your institution
How to buy a telescope for your institution by Dr. Frank Melsheimer DFM Engineering, Inc. 1035 Delaware Avenue Longmont, Colorado 80501 phone 303-678-8143 fax 303-772-9411 www.dfmengineering.com Table
More informationUVC LEDs for. Environmental Monitoring
UVC LEDs for Environmental Monitoring Environmental monitoring relies extensively on molecular spectroscopy for tracking air quality, water and wastewater quality, and detecting hazardous substances. Advances
More informationFTIR Instrumentation
FTIR Instrumentation Adopted from the FTIR lab instruction by H.-N. Hsieh, New Jersey Institute of Technology: http://www-ec.njit.edu/~hsieh/ene669/ftir.html 1. IR Instrumentation Two types of instrumentation
More informationExtreme-AO for GMT. Center for Astronomical Adaptive Optics, University of Arizona Subaru Telescope, National Astronomical Observatory of Japan
Extreme-AO for GMT Olivier Guyon Center for Astronomical Adaptive Optics, University of Arizona Subaru Telescope, National Astronomical Observatory of Japan guyon@naoj.org 1 Extreme-AO for GMT: Key science
More informationChapter 1 Parts C. Robert Bagnell, Jr., Ph.D., 2012
Chapter 1 Parts C. Robert Bagnell, Jr., Ph.D., 2012 Figure 1.1 illustrates the parts of an upright compound microscope and indicates the terminology that I use in these notes. Figure 1.1. Parts of a Compound
More informationAlpy 600 User Guide. Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com)
Alpy 600 User Guide Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com) DC0016A : april 2013 Alpy 600 spectroscope User Guide Olivier Thizy (olivier.thizy@shelyak.com)
More informationA PHOTOGRAMMETRIC APPRAOCH FOR AUTOMATIC TRAFFIC ASSESSMENT USING CONVENTIONAL CCTV CAMERA
A PHOTOGRAMMETRIC APPRAOCH FOR AUTOMATIC TRAFFIC ASSESSMENT USING CONVENTIONAL CCTV CAMERA N. Zarrinpanjeh a, F. Dadrassjavan b, H. Fattahi c * a Islamic Azad University of Qazvin - nzarrin@qiau.ac.ir
More informationHigh Resolution Planetary Imaging
High Resolution Planetary Imaging Fighting the Atmosphere Getting out of the Atmosphere Adaptive Optics Lucky Imaging Lucky Imaging is the process of capturing planets using a CCD video camera. A software
More informationOrigins of the Cosmos Summer 2016. Pre-course assessment
Origins of the Cosmos Summer 2016 Pre-course assessment In order to grant two graduate credits for the workshop, we do require you to spend some hours before arriving at Penn State. We encourage all of
More informationLNG Monitoring. Fiber-Optic Leakage Detection System. Pipeline leakage detection. Regasification and liquefaction monitoring
LNG Monitoring Fiber-Optic Leakage Detection System Pipeline leakage detection Regasification and liquefaction monitoring Tank annulus and base slab monitoring Spill containment control Intelligent Solutions
More informationEmail: tjohn@mail.nplindia.ernet.in
USE OF VIRTUAL INSTRUMENTS IN RADIO AND ATMOSPHERIC EXPERIMENTS P.N. VIJAYAKUMAR, THOMAS JOHN AND S.C. GARG RADIO AND ATMOSPHERIC SCIENCE DIVISION, NATIONAL PHYSICAL LABORATORY, NEW DELHI 110012, INDIA
More informationWAVELENGTH OF LIGHT - DIFFRACTION GRATING
PURPOSE In this experiment we will use the diffraction grating and the spectrometer to measure wavelengths in the mercury spectrum. THEORY A diffraction grating is essentially a series of parallel equidistant
More informationHigh Resolution Planetary Imaging Workflow
High Resolution Planetary Imaging Workflow Fighting the Atmosphere Getting out of the Atmosphere Adaptive Optics Lucky Imaging Lucky Imaging is the process of capturing planets using a CCD video camera.
More informationATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.
1 ATOMIC SPECTRA Objective: To measure the wavelengths of visible light emitted by atomic hydrogen and verify the measured wavelengths against those predicted by quantum theory. To identify an unknown
More informationPlanning Observations
Lab 6: Eclipsing Binary Stars (Due: 2008 Apr 23) Binary Stars Binary stars are systems in which two stars orbit each other under their mutual gravitational interaction. It is commonly claimed that most
More informationGetting Started emacs.cshrc & :+/usr/local/classes/astr1030/astron/ source.cshrc cd /usr/local/classes/astr1030 idl .compile ccdlab2 ccdlab2 exit
Getting Started You will be looking at a series of CCD images on the computer. A widget has been designed to help you view and manipulate the images. Here s how to get your computer up and running: (1)
More informationTriple Spec 4 Risk Assessment Table
Notes: 1. "Prob" is the probability that an event will occur, with 1 being the lowest and 5 the highest 2. "Impact" is the result of the event's occurring, and the overall effect on the project 3. Prob
More informationLaboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control
More informationIntroduction to reflective aberration corrected holographic diffraction gratings
Introduction to reflective aberration corrected holographic diffraction gratings By Steve Slutter, Wu Jiang, and Olivier Nicolle The reflective diffraction grating is the heart of most spectroscopy systems
More informationID Objective Requirements Description of Test Date & Examiner 15 Verify that the optics?? OMC
NAOMI OMC/NCU Acceptance Tests at the University of Durham ATC Document number AOW/GEN/RAH/15.0/06/00 OMC/NCU acceptance tests DRAFT (Version date: 2 nd June 2000) wht-naomi-44 The ID numbers are those
More informationPlanetary Imaging Workshop Larry Owens
Planetary Imaging Workshop Larry Owens Lowell Observatory, 1971-1973 Backyard Telescope, 2005 How is it possible? How is it done? Lowell Observatory Sequence,1971 Acquisition E-X-P-E-R-I-M-E-N-T-A-T-I-O-N!
More informationHigh Resolution Imaging of Satellites with Ground-Based 10-m Astronomical Telescopes
UCRL-TR-227709 High Resolution Imaging of Satellites with Ground-Based 10-m Astronomical Telescopes C. Marois February 2, 2007 Disclaimer This document was prepared as an account of work sponsored by an
More informationAutoguiding. Today and Tomorrow. Tom Krajci Astrokolkhoz (АСТРОКОЛХОЗ) Observatory, Cloudcroft, NM Elevation 9,440ft
Autoguiding Today and Tomorrow. Tom Krajci Astrokolkhoz (АСТРОКОЛХОЗ) Observatory, Cloudcroft, NM Elevation 9,440ft Overview Traditional autoguiding Faster correction methods Abandoning autoguiding Optical
More informationThe Wide Field Cassegrain: Exploring Solution Space
The Wide Field Cassegrain: Exploring Solution Space Peter Ceravolo Ceravolo Optical Systems www.ceravolo.com peter@ceravolo.com Abstract This article illustrates the use of an internal aperture stop in
More informationSpectral Measurement Solutions for Industry and Research
Spectral Measurement Solutions for Industry and Research Hamamatsu Photonics offers a comprehensive range of products for spectroscopic applications, covering the, Visible and Infrared regions for Industrial,
More informationSpectrophotometry of Ap Stars
Spectrophotometry of Ap Stars ASTRA Status Report Barry Smalley Astrophysics Group Keele University Staffordshire United Kingdom bs@astro.keele.ac.uk What is Spectrophotometry? Spectroscopy through a wide
More informationSIGNAL GENERATORS and OSCILLOSCOPE CALIBRATION
1 SIGNAL GENERATORS and OSCILLOSCOPE CALIBRATION By Lannes S. Purnell FLUKE CORPORATION 2 This paper shows how standard signal generators can be used as leveled sine wave sources for calibrating oscilloscopes.
More informationOne Degree Imager Pipeline Software and Archive Science Requirements Document
One Degree Imager Pipeline Software and Archive Science Requirements Document Version 1.5: 7/23/09!Ian!Dell(Antonio-!Daniel!Durand-!Daniel!1arbeck-!5nut!Olsen-!8ohn!Sal;er! Final!Draft!>dition?!Pierre!Aartin!
More informationLSST Data Management System Applications Layer Simulated Data Needs Description: Simulation Needs for DC3
LSST Data Management System Applications Layer Simulated Data Needs Description: Simulation Needs for DC3 Draft 25 September 2008 A joint document from the LSST Data Management Team and Image Simulation
More informationHigh Resolution Spatial Electroluminescence Imaging of Photovoltaic Modules
High Resolution Spatial Electroluminescence Imaging of Photovoltaic Modules Abstract J.L. Crozier, E.E. van Dyk, F.J. Vorster Nelson Mandela Metropolitan University Electroluminescence (EL) is a useful
More information- the. or may. scales on. Butterfly wing. magnified about 75 times.
Lecture Notes (Applications of Diffraction) Intro: - the iridescent colors seen in many beetles is due to diffraction of light rays hitting the small groovess of its exoskeleton - these ridges are only
More informationBrookhaven Magnet Division - Nuclear Physics Program Support Activities
Brookhaven - Nuclear Physics Program Support Activities Spin Program support E-Cooling R&D RIA RHIC Operations Support Funding AGS Warm Siberian Snake AGS Warm Snake Magnetic element designed and built
More informationPlaneWave CDK Telescope Instructions CDK12.5, 17, 20 and 24
PlaneWave CDK Telescope Instructions CDK12.5, 17, 20 and 24 V112712 1 Collimation and Secondary Spacing Procedure The CDK optical design has four optical elements shown in Figure 1. The primary mirror
More informationQHY (5L-II-M) CCD camera for video meteor observation
Proceedings of the IMC, Mistelbach, 2015 85 QHY (5L-II-M) CCD camera for video meteor observation Matej Korec Maximilian Hell Observatory & Planetarium korec@planetarium.sk A new digital camera and lens
More informationSPECTROSCOPY. Light interacting with matter as an analytical tool
SPECTROSCOPY Light interacting with matter as an analytical tool Electronic Excitation by UV/Vis Spectroscopy : X-ray: core electron excitation UV: valance electronic excitation IR: molecular vibrations
More informationAnna Serdyuchenko, Victor Gorshelev, Mark Weber John P. Burrows University of Bremen, Institute for Environmental Physics
Anna Serdyuchenko, Victor Gorshelev, Mark Weber John P. Burrows University of Bremen, Institute for Environmental Physics 3-5 June 2013 ACSO meeting WMO Geneva, Switzerland 1 Graphics: DLR-IMF 3-5 June
More informationC/KOSMOS Work Breakdown Structure Summary
C/OSMOS Work Breakdown Structure Summary Version 2.3 January 13, 2011 Version Date Changes 1.8 November 19, 2009 Final version prior to issuing contract 1.9 December 8, 2009 Added documentation control
More informationThe Balloon Experimental Twin Telescope for Infrared Interferometry (BETTII)
The Balloon Experimental Twin Telescope for Infrared Interferometry (BETTII) Dr. Stephen Rinehart NASA s Goddard Space Flight Center Laboratory for Observational Cosmology What is BETTII? As proposed,
More informationSpatially resolved spectroscopy of the exoplanet HR 8799 c
Spatially resolved spectroscopy of the exoplanet HR 8799 c M. Janson 1,4, C. Bergfors 2, M. Goto 2, W. Brandner 2, D. Lafrenière 3 janson@astro.utoronto.ca ABSTRACT HR 8799 is a multi-planet system detected
More informationSSO Transmission Grating Spectrograph (TGS) User s Guide
SSO Transmission Grating Spectrograph (TGS) User s Guide The Rigel TGS User s Guide available online explains how a transmission grating spectrograph (TGS) works and how efficient they are. Please refer
More informationAlpy calibration User Guide. Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com)
Alpy calibration User Guide Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com) DC0018A : april 2013 Alpy calibration module User Guide Olivier Thizy (olivier.thizy@shelyak.com)
More informationYour first. Buying a scope for the first time can be daunting. We reveal what you shoud look for and how to get up and running.
telescope Your first Buying a scope for the first time can be daunting. We reveal what you shoud look for and how to get up and running. By Will ater what type of telescope should I buy? A good all-round
More informationRealization of a UV fisheye hyperspectral camera
Realization of a UV fisheye hyperspectral camera Valentina Caricato, Andrea Egidi, Marco Pisani and Massimo Zucco, INRIM Outline Purpose of the instrument Required specs Hyperspectral technique Optical
More informationError Budget Tree for the ASTRI prototype: structure and mirrors
Code: ASTRI-SPEC-OAB-3100-002 Issue: 2 DATE 02/04/2012 Page: 1 Error Budget Tree for the ASTRI prototype: structure and mirrors Prepared by: Name: Rodolfo Canestrari Paolo Conconi Enrico Giro Gabriele
More informationSCORE Data Display and Analysis Software
SCORE Data Display and Analysis Software S. Giordano Rapporto nr.116 22/01/2009 SCORE DATA DISPLAY and ANALYSIS SOFTWARE SCORE Project prepared by S. Giordano authors S. Giordano reference issue 1.0 revision
More informationarxiv:0903.4116v1 [astro-ph.im] 24 Mar 2009
Astron. Nachr./AN xxx (xxxx) x, xxx xxx CTK - A new CCD Camera at the University Observatory Jena arxiv:0903.4116v1 [astro-ph.im] 24 Mar 2009 1. Introduction MARKUS MUGRAUER Astrophysikalisches Institut
More informationPUMPED Nd:YAG LASER. Last Revision: August 21, 2007
PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow
More informationA. Martinez, A. L. Klebaner, J. C. Theilacker, B. D. DeGraff, M. White and G. S. Johnson
FERMILAB-CONF-11-258-AD FERMILAB SRF CRYOMODULE OPERATIONAL EXPERIENCE A. Martinez, A. L. Klebaner, J. C. Theilacker, B. D. DeGraff, M. White and G. S. Johnson Fermi National Accelerator Laboratory Batavia,
More informationLUCIFER. LMS Version 1.60. LMS User Manual. Document Number: LBT-LUCIFER-MAN 030. Issue Number: Issue 1.0
LUCIFER LMS User Manual LMS Version 1.60 Document Number: LBT-LUCIFER-MAN 030 Issue Number: Issue 1.0 Issue Date: July 8, 2010 Prepared by: R. Hofmann, MPE Garching Contents 1 Introduction 1 1.1 Scope...............................................
More informationSoftware challenges in the implementation of large surveys: the case of J-PAS
Software challenges in the implementation of large surveys: the case of J-PAS 1/21 Paulo Penteado - IAG/USP pp.penteado@gmail.com http://www.ppenteado.net/ast/pp_lsst_201204.pdf (K. Taylor) (A. Fernández-Soto)
More informationFIRST GRADE 1 WEEK LESSON PLANS AND ACTIVITIES
FIRST GRADE 1 WEEK LESSON PLANS AND ACTIVITIES UNIVERSE CYCLE OVERVIEW OF FIRST GRADE UNIVERSE WEEK 1. PRE: Describing the Universe. LAB: Comparing and contrasting bodies that reflect light. POST: Exploring
More informationExperiment #5: Qualitative Absorption Spectroscopy
Experiment #5: Qualitative Absorption Spectroscopy One of the most important areas in the field of analytical chemistry is that of spectroscopy. In general terms, spectroscopy deals with the interactions
More informationHow To Process Data From A Casu.Com Computer System
CASU Processing: Overview and Updates for the VVV Survey Nicholas Walton Eduardo Gonalez-Solares, Simon Hodgkin, Mike Irwin (Institute of Astronomy) Pipeline Processing Summary Data organization (check
More informationLSST and the Cloud: Astro Collaboration in 2016 Tim Axelrod LSST Data Management Scientist
LSST and the Cloud: Astro Collaboration in 2016 Tim Axelrod LSST Data Management Scientist DERCAP Sydney, Australia, 2009 Overview of Presentation LSST - a large-scale Southern hemisphere optical survey
More information165 points. Name Date Period. Column B a. Cepheid variables b. luminosity c. RR Lyrae variables d. Sagittarius e. variable stars
Name Date Period 30 GALAXIES AND THE UNIVERSE SECTION 30.1 The Milky Way Galaxy In your textbook, read about discovering the Milky Way. (20 points) For each item in Column A, write the letter of the matching
More informationAstrophysics with Terabyte Datasets. Alex Szalay, JHU and Jim Gray, Microsoft Research
Astrophysics with Terabyte Datasets Alex Szalay, JHU and Jim Gray, Microsoft Research Living in an Exponential World Astronomers have a few hundred TB now 1 pixel (byte) / sq arc second ~ 4TB Multi-spectral,
More informationProton tracking for medical imaging and dosimetry
Proton tracking for medical imaging and dosimetry J.Taylor, P.Allport, G.Casse For the PRaVDA Consortium 1 Background and motivation - What is the PRaVDA experiment? - Why are we using Monte Carlo? GEANT4
More informationAlignment Laser System.
- O T 6 0 0 0 Alignment Laser System. The OT-6000. Multi -Target,Two Dimensional Alignment. Introducing the most powerful way to measure alignment at distances up to 300 feet. The OT-6000 Alignment Laser
More informationO6: The Diffraction Grating Spectrometer
2B30: PRACTICAL ASTROPHYSICS FORMAL REPORT: O6: The Diffraction Grating Spectrometer Adam Hill Lab partner: G. Evans Tutor: Dr. Peter Storey 1 Abstract The calibration of a diffraction grating spectrometer
More informationS2000 Spectrometer Data Sheet
Description The Ocean Optics OEM S2000 Spectrometer includes the linear CCD-array optical bench, plus the circuits necessary for spectrometer operation. The result is a compact, flexible system with no
More informationMultispectral stereo acquisition using 2 RGB cameras and color filters: color and disparity accuracy
Multispectral stereo acquisition using 2 RGB cameras and color filters: color and disparity accuracy (a) and Bernhard Hill (b) (a) Institute of Imaging and Computer Vision (b) Research Group Color and
More informationINFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING
INFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING Helmut Jorke, Markus Fritz INFITEC GmbH, Lise-Meitner-Straße 9, 89081 Ulm info@infitec.net Phone +49 731 550299 56 Fax _
More informationPerformance and results with the NIRSPEC echelle spectrograph on the Keck II Telescope
Performance and results with the NIRSPEC echelle spectrograph on the Keck II Telescope Ian S. McLean a, James R. Graham b, E. E. Becklin a, Donald F. Figer c, James Larkin a, N. Levenson d and Harry I.
More informationBuying Your First Telescope By Mike Usher
Buying Your First Telescope By Mike Usher The first thing to understand is that a telescope is a high quality optical device and high quality optical devices are not inexpensive. Second mortgages are not
More informationQUALITY CONTROL OF THE IUE FINAL ARCHIVE
QUALITY CONTROL OF THE IUE FINAL ARCHIVE N. Loiseau 1, E. Solano 1,M.Barylak 2 1 INSA/ESA IUE Observatory, Apdo. 50727, Villafranca del Castillo, 28080 Madrid (Spain). 2 ESA IUE Observatory, Apdo. 50727,
More informationILLUSTRATIVE EXAMPLE: Given: A = 3 and B = 4 if we now want the value of C=? C = 3 + 4 = 9 + 16 = 25 or 2
Forensic Spectral Anaylysis: Warm up! The study of triangles has been done since ancient times. Many of the early discoveries about triangles are still used today. We will only be concerned with the "right
More informationGP-B Telescope Measurement of Telescope Field of View P0454 Rev -
Page 1 SUGPB P0454 Rev Stanford University W.W. Hansen Experimental Physics Laboratory Gravity Probe B Relativity Mission Stanford, California 943054085 GPB Telescope Measurement of Telescope Field of
More informationWarning : HαT telescope must NOT be used for solar observation without additional filters. This is the user responsibility to check that his filter
For high resolution chromosphere observation and imaging in Hα band Warning : HαT telescope must NOT be used for solar observation without additional filters. This is the user responsibility to check that
More informationFinding Stars and Constellations Earth & Sky
Finding Stars and Constellations Earth & Sky Name: Introduction If you carefully watched the night sky over a period of time, you would notice that it s not always the same. There are certain changes that
More informationChallenges in DWDM System Spectral Analysis By Laurent Begin and Jim Nerschook
Challenges in DWDM System Spectral Analysis By Laurent Begin and Jim Nerschook TABLE OF CONTENTS: 1.0 Satisfying the Thirst for Bandwidth 02 2.0 The Solution, DWDM 02 3.0 Resolution 04 4.0 Wavelength Accuracy
More informationCCAT: Overview & Status
CCAT: Overview & Status Large Aperture Millimeter/Submillimeter Telescopes in the ALMA Era Osaka Prefecture University 12-13 Sept, 2011 Jeff Zivick CCAT Project Manager Cornell University Guiding Principles
More informationThe APOLLO cloud product statistics Web service The APOLLO cloud product statistics Web service
The APOLLO cloud product statistics Web service Introduction DLR and Transvalor are preparing a new Web service to disseminate the statistics of the APOLLO cloud physical parameters as a further help in
More informationOptical System Design
Optical System Design Robert E. Fischer CEO, OPTICS 1, Incorporated Biljana Tadic-Galeb Panavision Paul R. Yoder Consultant With contributions by Ranko Galeb Bernard C.Kress, Ph.D. Stephen C. McClain,
More informationRobot Perception Continued
Robot Perception Continued 1 Visual Perception Visual Odometry Reconstruction Recognition CS 685 11 Range Sensing strategies Active range sensors Ultrasound Laser range sensor Slides adopted from Siegwart
More informationPRODUCT SHEET. info@biopac.com support@biopac.com www.biopac.com
EYE TRACKING SYSTEMS BIOPAC offers an array of monocular and binocular eye tracking systems that are easily integrated with stimulus presentations, VR environments and other media. Systems Monocular Part
More informationTuning & Mass Calibration
Tuning & Mass Calibration 1 1 The Sample List Sample List Name Project Name 2 The sample list is the top level screen in the TurboMass Gold Software. Data storage is set up in PROJECT files and within
More informationUsing Photometric Data to Derive an HR Diagram for a Star Cluster
Using Photometric Data to Derive an HR Diagram for a Star Cluster In In this Activity, we will investigate: 1. How to use photometric data for an open cluster to derive an H-R Diagram for the stars and
More informationGRID AND PRISM SPECTROMETERS
FYSA230/2 GRID AND PRISM SPECTROMETERS 1. Introduction Electromagnetic radiation (e.g. visible light) experiences reflection, refraction, interference and diffraction phenomena when entering and passing
More informationAPPLICATION NOTE. Basler racer Migration Guide. Mechanics. www.baslerweb.com. Flexible Mount Concept. Housing
62 62 APPLICATION NOTE www.baslerweb.com Basler racer Migration Guide This paper describes what to consider when replacing the Basler L100 Camera Link or the Basler runner Gigabit Ethernet (GigE) line
More informationCharacterizing Digital Cameras with the Photon Transfer Curve
Characterizing Digital Cameras with the Photon Transfer Curve By: David Gardner Summit Imaging (All rights reserved) Introduction Purchasing a camera for high performance imaging applications is frequently
More informationGPS BLOCK IIF RUBIDIUM FREQUENCY STANDARD LIFE TEST
GPS BLOCK IIF RUBIDIUM FREQUENCY STANDARD LIFE TEST F. Vannicola, R. Beard, J. White, K. Senior, T. Kubik, D. Wilson U.S. Naval Research Laboratory 4555 Overlook Avenue, SW, Washington, DC 20375, USA E-mail:
More information