System Performance Metrics and Current Performance Status George Angeli.

Slides:



Advertisements
Similar presentations
A Crash Course in Radio Astronomy and Interferometry: 4
Advertisements

CMSC 2006 Orlando Active Alignment System for the LSST William J. Gressler LSST Project National Optical Astronomy Observatory (NOAO) Scott Sandwith New.
Systems Engineering Breakouts George Angeli. Tuesday 11am Current Commissioning Plans – Chuck Claver Revised commissioning timeline Development plans.
Practical Optics Class Opti696D, Fall Laser Bar Code Scanner Chunyu Zhao.
990901EIS_Opt.1 The Instrument: Optical Design Dr. John T. Mariska Data Coordination Scientist Naval Research Laboratory
Clouds and the Earth’s Radiant Energy System NASA Langley Research Center / Atmospheric Sciences Methodology to compare GERB- CERES filtered radiances.
Using DELPHI for Weak Lensing Measurements: Science Return and Mirror Size Jes Ford, JPL, UNR SURF /21/07 Mentor: Jason Rhodes Co-mentor: David Johnston.
Motion Tracking. Image Processing and Computer Vision: 82 Introduction Finding how objects have moved in an image sequence Movement in space Movement.
HST WFC3 IR channel: 1k x 1k HgCdTe detector, QE 80% 18 micron pixels (0.13”/pix), ~2’x2’ FOV Detector sensitivity engineered to cut off above 1.7 micron,
NGAO Instrumentation Overview September 2008 Updated Sean Adkins.
1 NGAO Instrumentation Studies Overview By Sean Adkins November 14, 2006.
LGS WFS Design Status & Issues Dekany, Delacroix, & Velur Caltech Optical Observatories.
WFS Preliminary design phase report I V. Velur, J. Bell, A. Moore, C. Neyman Design Meeting (Team meeting #10) Sept 17 th, 2007.
NGAO NGS WFS design review Caltech Optical Observatories 31 st March 2010.
PALM-3000 High-order Wavefront Sensor Update Christoph Baranec Team Meeting #9 10/22/2008.
VISTA pipelines summit pipeline: real time DQC verified raw product to Garching standard pipeline: instrumental signature removal, catalogue production,
LIM: Near IR from a mini-satellite Dani Maoz. HST WFC3 IR channel: 1k x 1k HgCdTe detector, QE 80% 18 micron pixels (0.13”/pix), ~2’x2’ FOV Detector.
LSST Wavefront Sensing Bo Xin Systems Analysis Scientist (LSSTPO) Chuck Claver, Ming liang, Srinivasan Chadrasekharan, George Angeli (LSST wavefront sensing.
1 Large Synoptic Survey Telescope Review Kirk Gilmore - SLAC DOE Review June 15, 2005.
CCD Image Processing: Issues & Solutions. Correction of Raw Image with Bias, Dark, Flat Images Flat Field Image Bias Image Output Image Dark Frame Raw.
NGAO Instrumentation Preliminary Design Phase Planning September 2008 Sean Adkins.
1 NGAO Science Instrument Reuse Part 1: NIRC2 NGAO IWG December 12, 2006.
1 K. Gilmore - SDW The Large Synoptic Survey Telescope (LSST) Status Summary Kirk Gilmore SLAC/KIPAC.
MCAO Adaptive Optics Module Mechanical Design Eric James.
The New Perturbation Physics Framework in PhoSim John Peterson En-Hsin Peng Chuck Claver Andy Rasmussen Steve Kahn Nov 2012.
01/28/05© 2005 University of Wisconsin Last Time Improving Monte Carlo Efficiency.
Laboratory prototype for the demonstration of sodium laser guide star wavefront sensing on the E-ELT Sexten Primary School July 2015 THE OUTCOME.
Science Impact of Sensor Effects or How well do we need to understand our CCDs? Tony Tyson.
The LSST Exposure Time Calculator was developed to model the effects of LSST design changes on signal-to-noise ratio and survey depth. The ETC utilizes.
STATUS REPORT OF FPC SPICA Task Force Meeting March 29, 2010 MATSUMOTO, Toshio (SNU)
Update to End to End LSST Science Simulation Garrett Jernigan and John Peterson December, 2004 Status of the Science End-to-End Simulator: 1. Sky Models.
1 FINAL DESIGN REVIEW | TUCSON, AZ | OCTOBER 21-25, 2013 Name of Meeting Location Date - Change in Slide Master Overview of LSST Tools and Simulations.
PACS SVR 22/23 June 2006 PACS FPU Subunits1 FM FPU Subunits A. Poglitsch.
NORDFORSK Summer School, La Palma, June-July 2006 NOT: Telescope and Instrumentation Michal I. Andersen & Heidi Korhonen Astrophysikalisches Institut Potsdam.
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
1 FINAL DESIGN REVIEW | TUCSON, AZ | OCTOBER 21-25, 2013 Name of Meeting Location Date - Change in Slide Master Title of Presentation Andrew Connolly LSST.
Strehl Ratio estimation. SR from H band images High Strehl PSF ->fitting with Zernike modes We suppose: No relevant loss of energy due to high modes (Z>36)
Asteroids Image Calibration and Setup Making a Lightcurve What is a Lightcurve? Cole Cook  Physics and Astronomy  University of Wisconsin-Eau Claire.
 PLATO PLAnetary Transits & Oscillations of stars Data onboard treatment PPLC study February 2009 on behalf of Reza Samadi for the PLATO data treatment.
Pachon Sky Camera Christopher Stubbs Chuck Claver Jan 25, 2014.
ASTEROSEISMOLOGY and SEARCH for EXOPLANETS Vienna - September 18 th 2001 Optical performance characterization Point Spread Function (PSF) : Telescope +
September 16, 2008LSST Camera F2F1 Camera Calibration Optical Configurations and Calculations Keith Bechtol Andy Scacco Allesandro Sonnenfeld.
Aldo Dell'Oro INAF- Observatory of Turin Detailed analysis of the signal from asteroids by GAIA and their size estimation Besançon November 6-7, 2003.
An evaluation method of the retrieved physical quantity deriving from the satellite remote sensing using analysis of variance in experimental design Mitsuhiro.
The Active Optics System S. Thomas and the AO team.
3.1.1 Optics, Optical Corrector, Mechanical Systems M. Johns, C. Claver.
SITE PARAMETERS RELEVANT FOR HIGH RESOLUTION IMAGING Marc Sarazin European Southern Observatory.
FLAO_01: FLAO system baseline & goal performance F. Quirós-Pacheco, L. Busoni FLAO system external review, Florence, 30/31 March 2009.
FELT 1 Study of the capability and configuration of a fixed mirror Extremely Large Telescope (FELT) Low cost path to large telescope Primary concern is.
March 31, 2000SPIE CONFERENCE 4007, MUNICH1 Principles, Performance and Limitations of Multi-conjugate Adaptive Optics F.Rigaut 1, B.Ellerbroek 1 and R.Flicker.
George Angeli 26 November, 2001 What Do We Need to Know about Wind for GSMT?
11-Jun-04 1 Joseph Hora & the IRAC instrument team Harvard-Smithsonian Center for Astrophysics The Infrared Array Camera (IRAC) on the Spitzer Space Telescope.
NIRISS NRM bad pixel tolerance analysis David Lafrenière 2012 February 21.
Charts for TPF-C workshop SNR for Nulling Coronagraph and Post Coron WFS M. Shao 9/28/06.
N A S A G O D D A R D S P A C E F L I G H T C E N T E R I n s t r u m e n t S y n t h e s i s a n d A n a l y s i s L a b o r a t o r y APS Formation Sensor.
1 WFC3 – Critical Science Review Science Driven CEIs Requirements.
ETC Block Diagram. Source Spectrum is derived from: Spectra Type –Stellar (50 stellar types) –Galaxies (elliptical, spiral) –QSO Luminosity Profile –point.
François Rigaut, Gemini Observatory GSMT SWG Meeting, LAX, 2003/03/06 François Rigaut, Gemini Observatory GSMT SWG Meeting, LAX, 2003/03/06 GSMT AO Simulations.
In conclusion the intensity level of the CCD is linear up to the saturation limit, but there is a spilling of charges well before the saturation if.
A. Ealet Berkeley, december Spectrograph calibration Determination of specifications Calibration strategy Note in
CCD Calibrations Eliminating noise and other sources of error.
B. Humensky 2/24/2012 CTA-SCT Mtg - SLAC
Lecture 14 AO System Optimization
Click to add title LSST Overview: Actuators, Perturbations, Controls, and Metrics George Angeli, Bo Xin, C. Claver, D. Neill Simulation Workshop SLAC,
Systems Engineering, Verification, and Commissioning for LSST George Z
NIRSpec pipeline concept Guido De Marchi, Tracy Beck, Torsten Böker
Charge Transfer Efficiency of Charge Coupled Device
First Assessments of EUVI Performance on STEREO SECCHI
Click to add title Planning for LSST Verification George Angeli LSST All Hands Meeting Tucson August 15, 2016.
Optics Alan Title, HMI-LMSAL Lead,
Presentation transcript:

System Performance Metrics and Current Performance Status George Angeli

Performance Metrics * Calibration update in-progress Updated estimates

Integrated Étendue − Basic definition − Extended definition Sensitivity Integrated étendue -Fill Factor (f F ) - accounts for losses in the field due to masks, bad pixels, charge stops -Sensitivity Factor (f S ) – accounts for sensitivity losses or gains due to throughput, image quality, read noise -Observing Efficiency Factor (f O ) – accounts for losses or gains in open shutter efficiency over the entire survey

Sensitivity Factor Not allocated - driven by allocable Technical Performance Metrics: – Image Quality – Throughput – Read noise For each band: Overall f s as time weighted sum Observing band (filter) Time Allocation e2v mAR Depth Margin over SRD Des. fSfS u band 6.7 % g band 9.7 % r band22.3 % i band22.3 % z band19.4 % y band19.4 % Overall 1.185

Evolution of Image Depth Reserve Reserve in LSR above SRD Minimum Specification See Chuck’s presentation for details Sensitivity factor relative to SRD minimum specs: P R O P O S E D

Image Depth Dependencies For each band: Image Quality Throughput and read noise r band Change since JIM Review

Image Quality Error Budget milliarcsecond (mas) Telescope reserve: 105 mas Camera reserve: 102 mas See Bo’s presentation for details of meeting this budget

Evolution of IQ System Reserve Charge diffusion contribution estimate reduced before FDR from 259 mas to 186 mas milliarcsecond (mas)

System Behavior PSF size and shape

Integrated System Model PSF size and shape Currently ZEMAX Preferably PhoSim

Deterministic effects – Optical design residual errors, – Diffraction effects due to the finite aperture and pupil obscuration, Deterministic effects randomized by environmental and operational parameters – Mirror support print through and lens gravitational deformations randomized through telescope zenith angle – Thermal deformations of optical surfaces and support structures randomized through ambient and local temperature Random processes – Dome and mirror seeing – Local actuator and sensor noise and drift (non-optical sensors) – Counting statistics – CCD sensor effects (solid state effects: diffusion, field dependencies, penetration depth, QE variations) – WFS measurement, estimation, and control errors – Material, fabrication, and installation errors; these become deterministic once the “as built” system is available Input Parameters (Perturbations)

FWHM across the field Ellipticity across the field Output Parameters (Metrics) Area weighted mean of 31 samples – Diffraction (FFT) PSF – Also track geometric PSF derived from spot RMS

Fiducial atmospheres (3) – Scaled to 0.44”, 0.6”, and 0.8” FWHM seeing on the aperture of LSST. Zenith angle range of 0˚- 65˚ – Statistical distribution derived from “standard” OpSim simulations. Temperature and pressure ranges as defined in the OSS as Normal Operating Conditions. – The temperature inside enclosed volumes, like the Camera, needs to be estimated from these environmental parameters. The expected temperature range of the detector, with assumed statistics Environmental Conditions

Transition the optical kernel to PhoSim Include missing instrumental perturbations – Most prominently sensor effects – In the process of implemented in PhoSim Improve AOS control laws and performance Establish a configuration adequate for science simulations – Linked or emulated AOS Future Work