SIRTF-IRS software Fred Lahuis Leiden 18 Nov 2002 (presented by Ewine van Dishoeck and Adwin Boogert, c2d meeting Dec. 11, 2002)

Slides:



Advertisements
Similar presentations
Pipeline flow. Pipeline flow- current preprocessing order (not necessarily the ideal one!) 0. Starting point 1. Try to measure (using calib. lamp) & undo.
Advertisements

Echelle Spectroscopy Dr Ray Stathakis, AAO. What is it? n Echelle spectroscopy is used to observe single objects at high spectral detail. n The spectrum.
Deconvolution Workshop – MPIfR, Bonn, D 2008 Dec 8 - page 1 HIFI Standing Waves Adwin Boogert, NHSC/IPAC, Pasadena, CA, USA.
MIPS Data Processing for SINGS George J. Bendo & Chad Engelbracht (A ''George's Adventures in Learning OpenOffice'' Presentation)
Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array Whoever North American.
SJC - 109/29/05IRAC Calibration Workshop Status of IRAC Artifact Corrector Sean Carey.
Echelle spectra reduction with IRAF*
FMOS Observations and Data 14 January 2004 FMOS Science Workshop.
U. Western Ontario Protoplanetary Disk Workshop, 19 May William Forrest (U of Rochester) Kyoung Hee Kim, Dan Watson, Ben Sargent (U. of R.) and.
Introduction to Spitzer and some applications Data products Pipelines Preliminary work K. Nilsson, J.M. Castro Cerón, J.P.U. Fynbo, D.J. Watson, J. Hjorth.
ADASS XVII - September, Software Modelling of IFU Spectrometers Nuria P. F. Lorente UK Astronomy Technology Centre Royal Observatory, Edinburgh,
Naoyuki Tamura (University of Durham) Expected Performance of FMOS ~ Estimation with Spectrum Simulator ~ Introduction of simulators  Examples of calculations.
Cophasing activities at Onera
Physical Modelling of Instruments Activities in ESO’s Instrumentation Division Florian Kerber, Paul Bristow.
0. To first order, the instrument is working very well ! 1.Evolution of the IR detector with time 2.Stability of the L channel 3.Saturation 4.Linearity.
Memorandam of the discussion on FMOS observations and data kicked off by Ian Lewis Masayuki Akiyama 14 January 2004 FMOS Science Workshop.
AAO Fibre Instrument Data Simulator 10 October 2011 ROE Workshop 2011 Michael Goodwin Tony Farrell Gayandhi De Silva Scott Smedley Australian Astronomical.
Beating Noise Observational Techniques ASTR 3010 Lecture 11 Textbook.
Jim Lewis and Guy Rixon, CASU. 24 April, 2001 Data-reduction Pipeline for the INT WFC: slide 1 The Data-reduction Pipeline for the INT Wide Field Camera.
Round Table Discussion Of Spectroscopic Processing & Products for the Scientific Legacy Nov 16, 2012HST Spec Pipeline & Legacy Products Round Table Kaiser,
IRS Data Products: An Update SINGS Team Meeting November 2002 Baltimore, MD L. Armus SIRTF Science Center.
September 14, Monday 4. Tools for Solar Observations-II Spectrographs. Measurements of the line shift.
14 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
Spectroscopic Observations (Massey & Hanson 2011, arXiv v2.pdf) Examples of Spectrographs Spectroscopy with CCDs Data Reduction and Calibration.
18 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
Proposal for a self-calibrating and instrument-independent MOS DRS Carlo Izzo.
ST–ECF UC, Dec 01 1 NGST support at the ST-ECF Bob Fosbury
KMOS Instrument Overview & Data Processing Richard Davies Max Planck Institute for Extraterrestrial Physics  What does KMOS do?  When will it do it?
Selection of the New COS/FUV Lifetime Position Cristina Oliveira Jan TIPS Meeting - COS/FUV Lifetime1.
Data products of GuoShouJing telescope(LAMOST) pipeline and current problems LUO LAMOST Workshop.
Source catalog generation Aim: Build the LAT source catalog (1, 3, 5 years) Jean Ballet, CEA SaclayGSFC, 29 June 2005 Four main functions: Find unknown.
Counting individual galaxies from deep mid-IR Spitzer surveys Giulia Rodighiero University of Padova Carlo Lari IRA Bologna Francesca Pozzi University.
MIRI Dither Patterns Christine H Chen. Dithering Goals 1.Mitigate the effect of bad pixels 2.Obtain sub-pixel sampling 3.Self-calibrate data if changing.
Herschel Open Time Cycle 1 DP workshop ESAC, March page 1 Spurs in HIFI data Colin Borys.
HARPS Data Flow System Christophe Lovis Geneva Observatory HARPS-N PDR, 6-7 December 2007, Cambridge MA.
The planet-forming zones of disks around solar- mass stars: a CRIRES evolutionary study VLT Large Program 24 nights.
MOS Data Reduction Michael Balogh University of Durham.
C2d Data flow diagram BCD from SSC Texas SAO Quality Analysis and Improved Calibrated Data Mapping team.
14 January Observational Astronomy SPECTROSCOPIC data reduction Piskunov & Valenti 2002, A&A 385, 1095.
The Critical Importance of Data Reduction Calibrations In the Interpretability of S-type Asteroid Spectra Michael J. Gaffey Space Studies Department University.
PACS NHSC Data Processing Workshop Aug 26-30, 2013 Page 1 SPIRE Spectrometer Data: Calibration Updates, User Data Reprocessing, and Other Issues Nanyao.
CUPID (Bob Narron)GRITS - May 14, CUPID “Customizable User Pipeline for IRS Data” Abstract: The CUPID package will allow users to run the Spitzer.
STScI Slitless Spectroscopy Workshop November 2010 aXe Advanced Topics – becoming more dextrous, using aXe with other instruments, making calibration.
Selection and Characterization of Interesting Grism Spectra Gerhardt R. Meurer The Johns Hopkins University Gerhardt R. Meurer The Johns Hopkins University.
NHSC HIFI DP workshop Caltech, 7-9 February page 1 Spurs in HIFI data.
STScI Calibration Workshop July 2010 Slitless Spectroscopy with HST Instruments Jeremy Walsh, Martin Kümmel & Harald Kuntschner, ST-ECF Former group.
New SPIRE features in HIPE 9.1 NHSC; Nov 28, 2012 PACS Page 1 What’s New in HIPE 9.1 ( SPIRE FTS) Nanyao Lu NHSC/IPAC (on behalf of the SPIRE ICC)
1 Core Data Processing Software Plan Review – University of Washington, Seattle, WA – Sept th Data Management XXVIII IAU General Assembly.
A. Ealet Berkeley, december Spectrograph calibration Determination of specifications Calibration strategy Note in
1 NHSC PACS NHSC/PACS Web Tutorials Running PACS photometer pipelines PACS-403 (for Hipe 13.0) Level 1 to Level 2.5 processing: The Unimap pipeline Prepared.
SINFONI data reduction using the ESO pipeline. Instrument design and its impact on the data (I) integral field spectrometer using mirrors brickwall pattern.
Adwin Boogert, NHSC/IPAC, Pasadena, CA, USA
Single Object Slitless Spectroscopy Simulations
A.Zanichelli, B.Garilli, M.Scodeggio, D.Rizzo
The Hubble Legacy Archive (HLA) Slitless Spectroscopy Project
JWST Pipeline Overview
Single Object & Time Series Spectroscopy with JWST NIRCam
Data Processing Status
JWST NIRCam Time Series Observations
COS FUV Flat Fields and Signal-to-Noise Characteristics
NIRSpec simulation data-package
Data Reduction and Analysis Techniques
ESAC 2017 JWST Workshop JWST User Documentation Hands on experience
THE LHIRES-III SPECTROGRAPH
What’s New in HIPE 10.0 (SPIRE FTS)
Integral Field Spectroscopy
UVIS Calibration Update
How we do Spectroscopy An Overview
Spectroscopic Observations (Massey & Hanson 2011, arXiv v2
X-ray high resolution spectra in the VO: the case of XMM-Newton RGS
Presentation transcript:

SIRTF-IRS software Fred Lahuis Leiden 18 Nov 2002 (presented by Ewine van Dishoeck and Adwin Boogert, c2d meeting Dec. 11, 2002)

IRS Instrument Low resolution R~ imaging spectrograph 1 st and 2 nd order SL Si:As micron LL Si:Sb micron High resolution R~600 echelle spectrograph order 11 to 20 SH Si:As micron LH Si:Sb micron

IRS images (128x128) Simulated single exposure of an extended source with an M82 + Circinus-like spectrum from mm, including cosmic rays. Simulated IRS SL image Sample IRS calibration files

IRS-ISO example IRS Low-Res IRS High-Res

IRS dataflow

IRS dataflow (cont’d) BCD products Lights-off Science pipeline Lights-on Science pipeline Science by legacy team TEXAS SSC Best effort Final delivery

SSC Pipeline Blackbox Products 2d images flatfielded BCD applied flatfield 1d spectrum nonimal extraction Flat-field is only controllable step Optimal extraction in SMART

SMART

SMART functionality " Read SSC data and handle complex projects (data volumes) " View and evaluate individual and series of files " Basic pixel arithmetic: add/subtract/multiple frames " Combine a series of images according to their quality " Spectral extraction for point and extended sources " (PU image analysis)  Combining spectra from different orders, modules, runs, … " Most of the ISAP features (line/BB/zodi fitting, photometry, line identification, dereddening) " Template fitting (source class identification, redshift) " Spectral maps (line ratio maps) " Interactive defringing

C2D Interactive Analysis SMART (legacy launch) project handler IRS image analysis optimal spectral extraction IRS calibration tools and data Defringing flatfield modification and robust sine wave fitting Modeling gas-phase molecules, disks, ices, solid state features C2D science pipeline scripts and data Spectral analysis/reduction tools zodiacal light, line-fitting,.... inspired by SWS IA, SMART-IDEA, ?

Catalogue 1. Spectra flux vs wavelength 2. Identification of features, where feasible 3. Flag for off-source emission, where feasible 4. Strengths of features 5. Classification of objects, cross refs 6. Complementary data Only 1-3 will be in catalog/deliveries to SSC; 4-6 TBC for final delivery

Instrumental fringes " Fabry-Perot effects on plane parallel surfaces within the instrument inside filters Plane mirrors detector surfaces Separations of a few mm are most efficient " Correction methods: FFT, bad Robust sine fitting Flatfield matching

Flatfield modification Minimize fringe residuals How? by modifying flatfield Fringe pattern changes per observation source offset in the slit shifts wavelength shifts fringe pattern source extent reduces effective resolution Stands or falls with the quality of the flatfield(s)

Flatfield modification II Determine phase shift and smooth/enhance factors for all orders Use smooth polynomial fit for phase shift and/or smooth/enhance factor?

Modflat pipeline issues #1 " Flat needs to be available, and in 1D approach extracted exactly the same way as science target. " In 1D approach: maximum sampling extracted spectrum crucial, in particular for highest echelle orders. " Smoothing fringe amplitude flat easier than enhancing. Flat used for Modflat should have highest possible resolution (point source). " Ideally, flat is available for each position in the slit, and best match with science observation is chosen from flat field 'database'. " For extended sources 2D version of Modflat may be considered: determine phase shift and smooth/enhance factors for each column. Adwin Boogert, IRS Fringing meeting Cornell, 30 August 2002

Modflat pipeline issues #2 " In case of extended source in combination with point source? Ideally extract spectrum of background and point source, and defringe independently, or simply subtract sky from point source. " Return header keywords: phase shift and amplitude reduction factor for each order. " 2D or not? May be better for extended source: apply modflat on each column. Point sources not expected to improve in 2D, what really matters is extraction at high sampling. Adwin Boogert, IRS Fringing meeting Cornell, 30 August 2002

Defringing: sine waves " Why use sine functions 'Simple' and robust algorithm Allows better estimation of fringe frequency than FFT Not limited by sampling or gaps in the spectrum Automatic mode using Bayesian evidence prevents overfitting " Goal: fringe artifact < 1% " Why? Most interesting science is in the weak features

Theory reflectance Computationally handy formula Implement a wavelength dependence of R and n and a x,y dependence of d Can we

Implementation Isolate fringes from continuum Find the strongest fringe components Compute the total fringe spectrum and return the defringed spectrum

Fringe characteristics Fringe parameters (frequency, amplitude and phase) relate to true physical parameters (refractive index, wafer thickness, reflectance and wavelength (source slit position)) ?..... what's next

Next " "Full" optical/physical model? " Parameters need to be extracted from the data " 2-D: requires optimal extraction and source modeling ".... " Will the data/calibration be good enough " We'll just have to try Good (self)calibration is crucial

Waterloo Conference First (to be) published IRS defringing paper

ISO-SWS Orion KL, Boonman et al. 2002

....