A.Zanichelli, B.Garilli, M.Scodeggio, D.Rizzo

Slides:



Advertisements
Similar presentations
GMOS Data Reduction Richard McDermid Gemini Data Reduction Workshop Tucson, July 2010.
Advertisements

GLAO instrument specifications and sensitivities
C. Beichman, Dimitra Touli, Gautam Vasisht, Roger Smith Tom Greene
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.
JWST IFUs and Data Tool Development Plans Tracy Beck JWST NIRSpec Instrument Scientist.
Echelle spectra reduction with IRAF*
FMOS Observations and Data 14 January 2004 FMOS Science Workshop.
AEOS Telescope + Image-Slicer/ Spectrograph Data Reduction and Results for June 8, 2006.
EPIC Calibration Meeting, Mallorca K. Dennerl, 2006 October 26 Suppression of the low-energy noise Suppression of the low-energy noise: an improved approach.
Extracting the Mystery from the Red Rectangle Meghan Canning, Zoran Ninkov, and Robert Slawson Chester Carlson Center for Imaging Science Rochester Institute.
Mercury’s Sodium Exosphere from Maui AEOS & Tohoku Observatory June 2006.
A. Ealet Berkeley, december Spectrometer simulation Note in ● Why we need it now ● What should.
Gemini Multi-Object Spectrograph (GMOS)
Naoyuki Tamura (University of Durham) Expected Performance of FMOS ~ Estimation with Spectrum Simulator ~ Introduction of simulators  Examples of calculations.
Memorandam of the discussion on FMOS observations and data kicked off by Ian Lewis Masayuki Akiyama 14 January 2004 FMOS Science Workshop.
Profile Measurement of HSX Plasma Using Thomson Scattering K. Zhai, F.S.B. Anderson, J. Canik, K. Likin, K. J. Willis, D.T. Anderson, HSX Plasma Laboratory,
HIFI Tutorial 3: Getting some basic science out A.P.Marston ESAC 27 June 2013.
NGC 2506 – a try for a spectroscopic study Ekaterina Atanasova Petr Kabath Christine Oppegaard Mª Carmen Sánchez Gil Tutor: Frédéric Royer 2nd NEON Archive.
Measuring the properties of QSO broad- line regions with the GMOS IFU. Randall Wayth with Matt O'Dowd & Rachel Webster.
Topic 10 - Image Analysis DIGITAL IMAGE PROCESSING Course 3624 Department of Physics and Astronomy Professor Bob Warwick.
Spectroscopic Observations (Massey & Hanson 2011, arXiv v2.pdf) Examples of Spectrographs Spectroscopy with CCDs Data Reduction and Calibration.
First results of the tests campaign in VISIBLE in VISIBLE for the demonstrator 12 October 2007 SNAP Collaboration Meeting Paris Marie-Hélène Aumeunier.
INTEGRAL FIELD SPECTROSCOPY AT THE VLT STAR (CLUSTER) FORMATION IN 3D : INTEGRAL FIELD SPECTROSCOPY AT THE VLT Markus Kissler-Patig (Instrument Scientist.
Integral Field Spectroscopy. David Lee, Anglo-Australian Observatory.
Proposal for a self-calibrating and instrument-independent MOS DRS Carlo Izzo.
PACS NHSC Data Processing Workshop – Pasadena 10 th - 14 th Sep 2012 SPIRE AOTs, Products and Quick Look Tools Bernhard Schulz NHSC/IPAC on behalf of the.
Data products of GuoShouJing telescope(LAMOST) pipeline and current problems LUO LAMOST Workshop.
Data Analysis Software Development Hisanori Furusawa ADC, NAOJ For HSC analysis software team 1.
Herschel Open Time Cycle 1 DP workshop ESAC, March page 1 Spurs in HIFI data Colin Borys.
MOS Data Reduction Michael Balogh University of Durham.
Practical applications: CCD spectroscopy Tracing path of 2-d spectrum across detector –Measuring position of spectrum on detector –Fitting a polynomial.
14 January Observational Astronomy SPECTROSCOPIC data reduction Piskunov & Valenti 2002, A&A 385, 1095.
Overview, Spectrometer Products and Processing Philosophy Phil Appleton on Behalf of PACS Team PACS IFU Spectrometer.
RAW DATA BIAS & DARK SUBTRACTION PIXEL-TO-PIXEL DQE CORR. LOCATE EXTR. WINDOW THROUGHPUT CORRECTION (incl. L-flat, blaze function, transmission of optics,
STScI Slitless Spectroscopy Workshop November 2010 aXe Advanced Topics – becoming more dextrous, using aXe with other instruments, making calibration.
NHSC HIFI DP workshop Caltech, 7-9 February page 1 Spurs in HIFI data.
UNIVERSIDAD COMPLUTENSE DE MADRID Grupo UCM de Astrofísica Instrumental y eXtragaláctica PRESENTADO POR: Raffaella Anna Marino COLABORADORES: A. Gil de.
2006/4/17-20 Extended 17 th SOT meeting M. Kubo (JAXA/ISAS), K. Ichimito, Y. Katsukawa (NAOJ), and SOT-team Comparison of FG and SP data from Sun test.
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
SINFONI data reduction using the ESO pipeline. Instrument design and its impact on the data (I) integral field spectrometer using mirrors brickwall pattern.
Single Object Spectroscopy and Time Series Observations with NIRSpec
Single Object Slitless Spectroscopy Simulations
NAC flat fielding and intensity calibration
JWST Pipeline Overview
Single Object & Time Series Spectroscopy with JWST NIRCam
Long-Slit Spectra Reduction with IRAF
NIRSpec pipeline concept Guido De Marchi, Tracy Beck, Torsten Böker
Data Processing Status
JWST NIRCam Time Series Observations
COS FUV Flat Fields and Signal-to-Noise Characteristics
Spectrophotometric calibration of the IFU spectrograph
The JWST Exposure Time Calculator
NIRSpec simulation data-package
ESAC 2017 JWST Workshop JWST User Documentation Hands on experience
SPIRE Spectrometer Data Reduction: Spectral Line Fitting
Summary Single Object & Time Series Spectroscopy Jeff Valenti JWST Mission Scientist Space Telescope Science Institute.
The Medium Resolution Spectrometer on behalf of the MRS team
The VIMOS IFU Pipeline Carlo Izzo.
What’s New in HIPE 10.0 (SPIRE FTS)
Integral Field Spectroscopy
Status of Equatorial CXRS System Development
Basics of Photometry.
NIR Spectroscopy at Gemini South
UVIS Calibration Update
Image Reduction and Analysis Facility
Modern Observational/Instrumentation Techniques Astronomy 500
Spectroscopic Observations (Massey & Hanson 2011, arXiv v2
X-ray high resolution spectra in the VO: the case of XMM-Newton RGS
Presentation transcript:

A.Zanichelli, B.Garilli, M.Scodeggio, D.Rizzo AUTOMATED DATA REDUCTION for the VIMOS INTEGRAL FIELD UNIT: how does it work? A.Zanichelli, B.Garilli, M.Scodeggio, D.Rizzo

IFU bundle and masks IFU Head

Why not use a “by hand” reduction? Huge amount of data (6400 spectra from each exposure) Complexity of IFU data IFU data reduction requires dedicated algorithms (with respect to MOS or long slit): cross-talk between spectra on the CCD calibration of fiber relative transmission sky determination and subtraction Need an automatic, dedicated IFU Data Reduction Pipeline

IFU First Light one quadrant, raw 1600 spectra Antennae Galaxy LR Red, 5 min. 0.67 arcsec/fiber

IFU Data Reduction Part of the VIMOS Data Reduction Software (imaging, MOS, IFU), developed in C and Python languages. As similar to VIMOS MOS data reduction as possible. Works on single quadrant (4 images are acquired from each VIMOS exposure) up to Data Cube reconstruction. Set of automatic procedures + some interactive functions. As for MOS, makes use of auxiliary tables needed for reduction (optical distortion models & c.).

The IFU Table The IFU Table has been built according to IFU construction specifications. For each fiber the IFU Table lists some fundamental parameters: correspondence between fiber position on the IFU head and spectrum on the detector fiber relative transmission measured by calibration procedures fiber profile parameters (X and Y FWHM of the spectrum on the CCD)

IFU Data Reduction Steps Sky determination and subtraction Photometric Calibration Build Data Cube Build reconstructed 2D Image 4 quadrants Bias and Flat Field correction Cross Talk correction Extract 2D spectrum + Wavelength calibration Extract 1D spectrum (no sky subtraction) Relative transmission correction

Cross-Talk Correction High density of spectra on the CCD  flux “contamination” from adjacent spectra Cross-Talk depends on: spectral flux fiber spatial profile For each fiber need to know fiber spatial profile parameters and shape At each cross dispersion cut: build spatial profile of each fiber compare with measured module profile apply flux correction

Fiber Relative Transmission Different fibers have different transmission efficiencies Relative transmission computed using sky lines Standard calibration of fiber relative transmission Image of twilight sky or image set in shift & stare mode fit sky lines + continuum (gaussian + 2 degrees polynomium) compute line flux and relative normalization Options: Use only 5577A sky line (stable) Use ALL possible sky lines and average If needed: further refinement on each scientific frame

Sky subtraction Stare observing mode: 400 spectra (work on pseudo-slits) Group fibers according to FWHM along dispersion For each group: Collapse spectra in wavelength, build flux distribution and compute mode fibers having fluxes below the mode are considered sky combine sky fibers, build Mean Sky for the group and subtract Shift & stare observing mode: work on single fiber spectra Combine exposures with rejection method Get a sky spectrum for each fiber and subtract

IFU DRS Final Steps Main IFU DRS products: set of 1D extracted, fully calibrated spectra + 3D data cube and 2D reconstructed image Data Cube: all the four quadrants must have been reduced fully calibrated 1D spectra are rearranged according to the IFU Table, to allow a spatially coherent reconstruction of the observed sky region 2D reconstructed image: collapsing data cube in wavelength: whole grism spectral range or user-selected, smaller range use interpolation/drizzling techniques

HDF South Through IFU

Interactive Tools Crowded fields: accurate sky subtraction automatic Data Reduction does not guarantee optimal sky subtraction on 2D reconstructed image, manually select fibers in sky regions build sky spectrum and subtract Spectra Co-addition on 2D reconstructed image, check for “extended” objects spectra from microlenses falling on the same object are summed Data Cube “slicing” select wavelength to get “monochromatic” image select range to get “narrow band” image

Conclusions IT WORKS…provided you have a very accurate calibration dataset!