NHSC/PACS Webinar. Aperture and pointing corrections for point sources

Size: px
Start display at page:

Download "NHSC/PACS Webinar. Aperture and pointing corrections for point sources"

Transcription

1 NHSC/PACS Webinar Aperture and pointing corrections for point sources D. Fadda December 13, 2012 page 1

2 Introduction This web-seminar will introduce you to the aperture correction and pointing/jitter correction for point sources. Pre-requisites Installing HIPE 10.0 on your computer PACS data reduction guide Spectroscopy: section page 2

3 Overview 0 Point sources 1 Aperture correction 2 Pointing/jitter correction 3 Case of non-central pixel page 3

4 What is the beam of Herschel? The beam of Herschel has been empirically derived in several key-wavelengths for all the 25 modules of the blue and red arrays. The pixel size is 9.4 x 9.4 and, even at the bluest wavelengths, approximately 30% of the flux falls out of the central pixel for a point source. In the red, the percentage could be bigger than 50%. On the top of that, pointing inaccuracies and jitter of the telescope add uncertainty on the total flux collected in the central pixel. In this case, unfortunately, a solution is available only in the case of bright sources. page 4

5 The beam The pixel size of the array is 9.4 x9.4. The FWHM varies at different wavelengths from 8 x8 in the blue to 12 x12 in the red. page 5

6 The empirical beam 75 μm 150 μm The dashed lines indicate the percentage of flux in the central spaxel and in the central 3x3 spaxels in the case of the empirical beam. Most of the flux is inside The 3x3 central spaxels. page 6

7 The PSF model The aperture correction has to take into account the totality of the flux not observed in the central spaxel. Direct observations are limited to a 30 arcmin radius and the outer parts are dominated by noise. For this reason, a PSF model is used to compute the fraction of flux seen in the central pixel. As shown, the flux fraction missed can be quite significant especially in the red. page 7

8 Aperture correction in the pipeline For point sources, the recommended way is to use the rebinned cube to measure the flux. If correctly planned, the source should be in the central pixel. You can use: extractspaxelspectrum to extract the spectrum of a spaxel in SimpleSpectrum format. Then use: pointsourcelosscorrection, to correct for the loss of flux using a PSF model. page 8

9 Aperture correction in the pipeline In the case the pixel with flux is the central one, the module extractcentralspectrum which combines extraction with aperture correction can be used: centralspectrum = extractcentralspectrum(slicedfinalcubes, \ slice=slice, nonans=1, width=0, \ applypointsourcecorrection=1, \ correct3x3=0, caltree=caltree) Choosing width=0, will apply a single median correction over the entire wavelength range. This is the recommended choice for line scan AOTs. The option correct3x3 is explained later. page 9

10 Pointing accuracy Herschel had a requirement of 1.5 arcsec pointing accuracy which was achieved in the year of observations. In the last year, the pointing has been improved to 1.0 arcsec. Pointing jitter requirement was of 0.3 arcsec/min. Occasionally, depending on the number of guide stars available, this value can be greater. Since such displacements can lead to substantial variations of the collected flux it is advisable to apply a correction. Unfortunately, it is possible to derive a correction only for bright sources with some flux in the central 3x3 spaxels. For calibration sources, already adding up the flux from the central 3x3 spaxels improve the reproducibility by a factor 2 wrt flux from the central pixel only. page 10

11 Pointing accuracy In case of point sources in the central spaxel, it is possible to Apply the so-called 3x3 correction. This takes into account the flux from the 3x3 central spaxels To correct for mispointing the flux of the central spaxel. Please, note that this correction can be applied only if there is measured flux in all the 3x3 central spaxels. centralspectrum = extractcentralspectrum(slicedfinalcubes, \ slice=slice, nonans=1, width=0, \ applypointsourcecorrection=1, \ Correct3x3=1, caltree=caltree) page 11

12 Non central pixel In the case the pixel with flux is not the central one, we have to first extract the pixel and the apply the aperture correction. This is available under scripts in HIPE 10. centralspectrum = extractspaxelspectrum( slicedfinalcubes, slice=slice, spaxelx=spaxelx, spaxely=spaxely) centralspectrum = pointsourcelosscorrection( centralspectrum, caltree=caltree) page 12

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for CHOP/NOD Mode. PACS-301 Level 0 to 1 processing

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for CHOP/NOD Mode. PACS-301 Level 0 to 1 processing NHSC/PACS s Running the PACS Spectrometer pipeline for CHOP/NOD Mode page 1 PACS-301 Level 0 to 1 processing Prepared by Dario Fadda September 2012 Introduction This tutorial will guide you through the

More information

Extracting Photometry from SPIRE Maps

Extracting Photometry from SPIRE Maps NHSC SPIRE Point Source Spectroscopy Webinar 21 March 2012 Extracting Photometry from SPIRE Maps David Shupe, Bernhard Schulz, Kevin Xu on behalf of the SPIRE ICC PACS NHSC SPIRE Point Source Photometry

More information

PACS data reduction for the PEP deep extragalactic survey

PACS data reduction for the PEP deep extragalactic survey PACS data reduction for the PEP deep extragalactic survey D. Lutz, P. Popesso, S. Berta and the PEP reduction team Herschel map making workshop Jan 28-31 2013 Ugly! Boring! how do we detect yet more of

More information

SPIRE Broad-Band Photometry Extraction

SPIRE Broad-Band Photometry Extraction SPIRE Broad-Band Photometry Extraction Bernhard Schulz (NHSC/IPAC) on behalf of the SPIRE ICC, the HSC and the NHSC Contents Point Source Photometry Choices Extended gain correction factors Zero-point

More information

PACS SED and large range scan AOT release note PACS SED and large range scan AOT release note

PACS SED and large range scan AOT release note PACS SED and large range scan AOT release note Page: 1 of 16 PACS SED and large range scan AOT PICC-KL-TN-039 Prepared by Bart Vandenbussche Alessandra Contursi Helmut Feuchtgruber Ulrich Klaas Albrecht Poglitsch Pierre Royer Roland Vavrek Approved

More information

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for unchopped line mode. PACS-303 Level 0 to 2 processing

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for unchopped line mode. PACS-303 Level 0 to 2 processing NHSC/PACS s Running the PACS Spectrometer pipeline for unchopped line mode PACS-303 Level 0 to 2 processing Prepared by Dario Fadda April 2014 page 1 Introduction This tutorial will guide you through the

More information

PACS photometry on extended sources

PACS photometry on extended sources PACS photometry on extended sources Total flux experiments Bruno Altieri on behalf of Marc Sauvage 1. Point-source photometry status 2. Prospect on extended emission photometry from theory 3. Results from

More information

Photometry from Herschel maps Ivan Valtchanov

Photometry from Herschel maps Ivan Valtchanov Photometry from Herschel maps Ivan Valtchanov SPIRE Instrument and Calibration Scientist Herschel Science Centre, ESAC, ESA Herschel and ALMA: PACS 1. Two broad-band photometers with Herschel: a. PACS:

More information

Basic principles of PACS photometer data reduc7on

Basic principles of PACS photometer data reduc7on Basic principles of PACS photometer data reduc7on B. Altieri, HSC/ESAC November 2012 B. Altieri HSC/ESAC November 2012 Slide 1 PACS photometer Two filled bolometer arrays in dual band imaging: 64x32 pixels

More information

NHSC/PACS Webinar PACS Point Source Photometry. Aperture Photometry and Photometric Uncertain5es. Roberta Paladini NHSC PACS.

NHSC/PACS Webinar PACS Point Source Photometry. Aperture Photometry and Photometric Uncertain5es. Roberta Paladini NHSC PACS. NHSC/PACS Webinar PACS Point Source Photometry Aperture Photometry and Photometric Uncertain5es Roberta Paladini July 2012 1 Content I Point- source aperture photometry in HIPE II Calibra=on errors III

More information

First Summary of Neptune Beam Measurements

First Summary of Neptune Beam Measurements First Summary of Neptune Beam Measurements Background subtraction with modified telescope normalization for asymmetric chopping sans nod works very well; offset in Gaussian fit is

More information

QUICK-START GUIDE TO HERSCHEL PACS THE PHOTOMETER. Katrina Exter HERSCHEL-HSC-DOC-2151, version 1.0, February 28, 2017

QUICK-START GUIDE TO HERSCHEL PACS THE PHOTOMETER. Katrina Exter HERSCHEL-HSC-DOC-2151, version 1.0, February 28, 2017 QUICK-START GUIDE TO HERSCHEL PACS THE PHOTOMETER Katrina Exter HERSCHEL-HSC-DOC-2151, version 1.0, February 28, 2017 Contents The PACS photometer 2 Photometer beams 4 Photometer observing modes (AOTs)

More information

Update on SPIRE Photometer Pipeline

Update on SPIRE Photometer Pipeline Update on SPIRE Photometer Pipeline Kevin Xu NHSC/IPAC on behalf of the SPIRE ICC page 1 What s New in HIPE 9.1 Improved map-making, with destriper in standard processing Electrical crosstalk correction

More information

JCMT HETERODYNE DR FROM DATA TO SCIENCE

JCMT HETERODYNE DR FROM DATA TO SCIENCE JCMT HETERODYNE DR FROM DATA TO SCIENCE https://proposals.eaobservatory.org/ JCMT HETERODYNE - SHANGHAI WORKSHOP OCTOBER 2016 JCMT HETERODYNE INSTRUMENTATION www.eaobservatory.org/jcmt/science/reductionanalysis-tutorials/

More information

Issues with Photometer Data & How to Resolve them with HIPE Tools

Issues with Photometer Data & How to Resolve them with HIPE Tools Issues with Photometer Data & How to Resolve them with HIPE Tools Kevin Xu NHSC/IPAC on behalf of the SPIRE ICC Known Issues New Flux Calibration in HIPE 11 Cooler Burps Glitches Missed Thermistor Signal

More information

The Heterodyne Instrument for the Far-Infrared (HIFI) and its data

The Heterodyne Instrument for the Far-Infrared (HIFI) and its data The Heterodyne Instrument for the Far-Infrared (HIFI) and its data D. Teyssier ESAC 28/10/2016 Outline 1. What was HIFI and how did it work 2. What was HIFI good for science cases 3. The HIFI calibration

More information

OSIRIS Hackathon. May 4-6, 2016

OSIRIS Hackathon. May 4-6, 2016 OSIRIS Hackathon May 4-6, 2016 Wednesday Schedule 9:30 am - 10 am - Goals and organization 10 am - 11:30 am - Breakout groups discuss plans C-code debugging/coding Greg, Shelley, James, Anna, Jim Running

More information

This release contains deep Y-band images of the UDS field and the extracted source catalogue.

This release contains deep Y-band images of the UDS field and the extracted source catalogue. ESO Phase 3 Data Release Description Data Collection HUGS_UDS_Y Release Number 1 Data Provider Adriano Fontana Date 22.09.2014 Abstract HUGS (an acronym for Hawk-I UDS and GOODS Survey) is a ultra deep

More information

Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude

Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude Hans Kjeldsen, Torben Arentoft and Jørgen Christensen-Dalsgaard KASOC, Stellar Astrophysics Centre, Aarhus

More information

TIRCAM2 (TIFR Near Infrared Imaging Camera - 3.6m Devasthal Optical Telescope (DOT)

TIRCAM2 (TIFR Near Infrared Imaging Camera - 3.6m Devasthal Optical Telescope (DOT) TIRCAM2 (TIFR Near Infrared Imaging Camera - II) @ 3.6m Devasthal Optical Telescope (DOT) (ver 4.0 June 2017) TIRCAM2 (TIFR Near Infrared Imaging Camera - II) is a closed cycle cooled imager that has been

More information

The predicted performance of the ACS coronagraph

The predicted performance of the ACS coronagraph Instrument Science Report ACS 2000-04 The predicted performance of the ACS coronagraph John Krist March 30, 2000 ABSTRACT The Aberrated Beam Coronagraph (ABC) on the Advanced Camera for Surveys (ACS) has

More information

F/48 Slit Spectroscopy

F/48 Slit Spectroscopy 1997 HST Calibration Workshop Space Telescope Science Institute, 1997 S. Casertano, et al., eds. F/48 Slit Spectroscopy R. Jedrzejewski & M. Voit Space Telescope Science Institute, Baltimore, MD 21218

More information

AKARI FIS Data User Manual

AKARI FIS Data User Manual AKARI FIS Data User Manual Version 1.3 Eva Verdugo 1, Issei Yamamura 2 and Chris Pearson 1,2 with contributions from: Mai Shirahata 2, Shuji Matsuura 2,YokoOkada 2, Sin itirou Makiuti 2, Noriko Murakami

More information

Guide to observation planning with GREAT

Guide to observation planning with GREAT Guide to observation planning with GREAT G. Sandell GREAT is a heterodyne receiver designed to observe spectral lines in the THz region with high spectral resolution and sensitivity. Heterodyne receivers

More information

Reference and User Manual May, 2015 revision - 3

Reference and User Manual May, 2015 revision - 3 Reference and User Manual May, 2015 revision - 3 Innovations Foresight 2015 - Powered by Alcor System 1 For any improvement and suggestions, please contact customerservice@innovationsforesight.com Some

More information

GPI INSTRUMENT PAGES

GPI INSTRUMENT PAGES GPI INSTRUMENT PAGES This document presents a snapshot of the GPI Instrument web pages as of the date of the call for letters of intent. Please consult the GPI web pages themselves for up to the minute

More information

Simulations of the STIS CCD Clear Imaging Mode PSF

Simulations of the STIS CCD Clear Imaging Mode PSF 1997 HST Calibration Workshop Space Telescope Science Institute, 1997 S. Casertano, et al., eds. Simulations of the STIS CCD Clear Imaging Mode PSF R.H. Cornett Hughes STX, Code 681, NASA/GSFC, Greenbelt

More information

Stellar Photometry: I. Measuring. Ast 401/Phy 580 Fall 2014

Stellar Photometry: I. Measuring. Ast 401/Phy 580 Fall 2014 What s Left (Today): Introduction to Photometry Nov 10 Photometry I/Spectra I Nov 12 Spectra II Nov 17 Guest lecture on IR by Trilling Nov 19 Radio lecture by Hunter Nov 24 Canceled Nov 26 Thanksgiving

More information

arxiv: v1 [astro-ph.im] 18 Nov 2012

arxiv: v1 [astro-ph.im] 18 Nov 2012 Astronomy & Astrophysics manuscript no. hpf psf final c ESO 2014 January 9, 2014 The effect of the high-pass filter data reduction technique on the Herschel PACS Photometer PSF and noise. P. Popesso 1,

More information

A PSF-fitting Photometry Pipeline for Crowded Under-sampled Fields. M. Marengo & Jillian Neeley Iowa State University

A PSF-fitting Photometry Pipeline for Crowded Under-sampled Fields. M. Marengo & Jillian Neeley Iowa State University A PSF-fitting Photometry Pipeline for Crowded Under-sampled Fields M. Marengo & Jillian Neeley Iowa State University What, and Why Developed to extract globular cluster photometry for Spitzer/IRAC Carnegie

More information

High Contrast Imaging using WFC3/IR

High Contrast Imaging using WFC3/IR SPACE TELESCOPE SCIENCE INSTITUTE Operated for NASA by AURA WFC3 Instrument Science Report 2011-07 High Contrast Imaging using WFC3/IR A. Rajan, R. Soummer, J.B. Hagan, R.L. Gilliland, L. Pueyo February

More information

NHSC/PACS Web Tutorials Running PACS photometer pipelines PACS-201

NHSC/PACS Web Tutorials Running PACS photometer pipelines PACS-201 NHSC/PACS Web Tutorials Running PACS photometer pipelines PACS 201 Level 0 to Level 1 processing: From raw to calibrated data cubes Prepared by Nicolas Billot February 2011 - page 1 Introduc=on NHSC PACS

More information

Chapter 8 FOC Data Analysis

Chapter 8 FOC Data Analysis Chapter 8 FOC Data Analysis In This Chapter... Photometry / 8-1 Astrometry / 8-6 Polarimetry / 8-7 Objective-Prism Spectroscopy / 8-10 Long-Slit Spectroscopy / 8-14 Summary of FOC Accuracies / 8-17 The

More information

Flux Calibration Monitoring: WFC3/IR G102 and G141 Grisms

Flux Calibration Monitoring: WFC3/IR G102 and G141 Grisms Instrument Science Report WFC3 2014-01 Flux Calibration Monitoring: WFC3/IR and Grisms Janice C. Lee, Norbert Pirzkal, Bryan Hilbert January 24, 2014 ABSTRACT As part of the regular WFC3 flux calibration

More information

Determination of the Focal Width with the Focal Width Script

Determination of the Focal Width with the Focal Width Script Tutorial Determination of the Focal Width with the Focal Width Script Summary This tutorial shows step-by-step, how to determine the Point Spread Function (PSF) of a microscopic system using the Focal

More information

SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals

SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals Published on SOAR (http://www.ctio.noao.edu/soar) Home > SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals SOAR Integral Field Spectrograph (SIFS): Call for Science Verification

More information

Next Generation Very Large Array Memo No. 47 Resolution and Sensitivity of ngvla-revb. C.L. Carilli (NRAO)

Next Generation Very Large Array Memo No. 47 Resolution and Sensitivity of ngvla-revb. C.L. Carilli (NRAO) Next Generation Very Large Array Memo No. 47 Resolution and Sensitivity of ngvla-revb C.L. Carilli (NRAO) Abstract I investigate the noise performance vs. resolution for the new ngvlarevb configuration.

More information

FLAT FIELD DETERMINATIONS USING AN ISOLATED POINT SOURCE

FLAT FIELD DETERMINATIONS USING AN ISOLATED POINT SOURCE Instrument Science Report ACS 2015-07 FLAT FIELD DETERMINATIONS USING AN ISOLATED POINT SOURCE R. C. Bohlin and Norman Grogin 2015 August ABSTRACT The traditional method of measuring ACS flat fields (FF)

More information

Southern African Large Telescope. RSS UW Commissioning Activities,

Southern African Large Telescope. RSS UW Commissioning Activities, Southern African Large Telescope RSS UW Commissioning Activities, 2014-1 Kenneth Nordsieck University of Wisconsin v 1.1 5 Nov, 2014 Change History Rev Date Description 1.0 3 Nov, 2014 Original 1.1 5 Nov,

More information

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist)

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist) MIRI The Mid-Infrared Instrument for the JWST ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist) 1 Summary MIRI overview, status and vital statistics. Sensitivity, saturation and

More information

You, too, can make useful and beautiful astronomical images at Mees: Lesson 1

You, too, can make useful and beautiful astronomical images at Mees: Lesson 1 You, too, can make useful and beautiful astronomical images at Mees: Lesson 1 Useful references: The Mees telescope startup/shutdown guide: http://www.pas.rochester.edu/~dmw/ast142/projects/chklist.pdf

More information

Comprehensive Vicarious Calibration and Characterization of a Small Satellite Constellation Using the Specular Array Calibration (SPARC) Method

Comprehensive Vicarious Calibration and Characterization of a Small Satellite Constellation Using the Specular Array Calibration (SPARC) Method This document does not contain technology or Technical Data controlled under either the U.S. International Traffic in Arms Regulations or the U.S. Export Administration Regulations. Comprehensive Vicarious

More information

ASD and Speckle Interferometry. Dave Rowe, CTO, PlaneWave Instruments

ASD and Speckle Interferometry. Dave Rowe, CTO, PlaneWave Instruments ASD and Speckle Interferometry Dave Rowe, CTO, PlaneWave Instruments Part 1: Modeling the Astronomical Image Static Dynamic Stochastic Start with Object, add Diffraction and Telescope Aberrations add Atmospheric

More information

NHSC/PACS Web Tutorials Running PACS photometer pipelines. PACS 201 (for Hipe 5.0) Level 0 to Level 1 processing: From raw to calibrated data cubes

NHSC/PACS Web Tutorials Running PACS photometer pipelines. PACS 201 (for Hipe 5.0) Level 0 to Level 1 processing: From raw to calibrated data cubes NHSC/PACS Web Tutorials Running PACS photometer pipelines PACS 201 (for Hipe 5.0) Level 0 to Level 1 processing: From raw to calibrated data cubes Prepared by Nicolas Billot and Roberta Paladini August

More information

ENGINEERING CHANGE ORDER ECO No. COS-058 Center for Astrophysics & Space Astronomy Date 2 March 2001 University of Colorado, Boulder Sheet 1 of 16

ENGINEERING CHANGE ORDER ECO No. COS-058 Center for Astrophysics & Space Astronomy Date 2 March 2001 University of Colorado, Boulder Sheet 1 of 16 University of Colorado, Boulder Sheet 1 of 16 Description of Change: 1. Section 2.1.1.2, p. 30 of Rev 10: The LSHUTINI macro was deleted some time ago, so the only remaining macro is to Move External Shutter.

More information

Exoplanet Imaging with the Giant Magellan Telescope

Exoplanet Imaging with the Giant Magellan Telescope Exoplanet Imaging with the Giant Magellan Telescope Johanan L. Codona Steward Observatory, University of Arizona, Tucson, AZ, USA 85721 ABSTRACT The proposed Giant Magellan Telescope (GMT) has a number

More information

Exo-planet transit spectroscopy with JWST/NIRSpec

Exo-planet transit spectroscopy with JWST/NIRSpec Exo-planet transit spectroscopy with JWST/NIRSpec P. Ferruit / S. Birkmann / B. Dorner / J. Valenti / J. Valenti / EXOPAG meeting 04/01/2014 G. Giardino / Slide #1 Table of contents Instrument overview

More information

Photometry. La Palma trip 2014 Lecture 2 Prof. S.C. Trager

Photometry. La Palma trip 2014 Lecture 2 Prof. S.C. Trager Photometry La Palma trip 2014 Lecture 2 Prof. S.C. Trager Photometry is the measurement of magnitude from images technically, it s the measurement of light, but astronomers use the above definition these

More information

SINGS: The Spitzer Infrared Nearby Galaxies Survey First Data Delivery October 2004 USER S GUIDE

SINGS: The Spitzer Infrared Nearby Galaxies Survey First Data Delivery October 2004 USER S GUIDE SINGS: The Spitzer Infrared Nearby Galaxies Survey First Data Delivery October 2004 USER S GUIDE 1. Introduction This document describes the first data delivery of the Spitzer Legacy program SINGS. It

More information

Photometry using CCDs

Photometry using CCDs Photometry using CCDs Signal-to-Noise Ratio (SNR) Instrumental & Standard Magnitudes Point Spread Function (PSF) Aperture Photometry & PSF Fitting Examples Some Old-Fashioned Photometers ! Arrangement

More information

LSST All-Sky IR Camera Cloud Monitoring Test Results

LSST All-Sky IR Camera Cloud Monitoring Test Results LSST All-Sky IR Camera Cloud Monitoring Test Results Jacques Sebag a, John Andrew a, Dimitri Klebe b, Ronald D. Blatherwick c a National Optical Astronomical Observatory, 950 N Cherry, Tucson AZ 85719

More information

CHAPTER 6 Exposure Time Calculations

CHAPTER 6 Exposure Time Calculations CHAPTER 6 Exposure Time Calculations In This Chapter... Overview / 75 Calculating NICMOS Imaging Sensitivities / 78 WWW Access to Imaging Tools / 83 Examples / 84 In this chapter we provide NICMOS-specific

More information

ALMA Phase Calibration, Phase Correction and the Water Vapour Radiometers

ALMA Phase Calibration, Phase Correction and the Water Vapour Radiometers ALMA Phase Calibration, Phase Correction and the Water Vapour Radiometers B. Nikolic 1, J. S. Richer 1, R. E. Hills 1,2 1 MRAO, Cavendish Lab., University of Cambridge 2 Joint ALMA Office, Santiago, Chile

More information

Segmented deformable mirrors for Ground layer Adaptive Optics

Segmented deformable mirrors for Ground layer Adaptive Optics Segmented deformable mirrors for Ground layer Adaptive Optics Edward Kibblewhite, University of Chicago Adaptive Photonics LLC Ground Layer AO Shack Hartmann Images of 5 guide stars in Steward Observatory

More information

Telescopes and their configurations. Quick review at the GO level

Telescopes and their configurations. Quick review at the GO level Telescopes and their configurations Quick review at the GO level Refraction & Reflection Light travels slower in denser material Speed depends on wavelength Image Formation real Focal Length (f) : Distance

More information

Wide-Band Imaging. Outline : CASS Radio Astronomy School Sept 2012 Narrabri, NSW, Australia. - What is wideband imaging?

Wide-Band Imaging. Outline : CASS Radio Astronomy School Sept 2012 Narrabri, NSW, Australia. - What is wideband imaging? Wide-Band Imaging 24-28 Sept 2012 Narrabri, NSW, Australia Outline : - What is wideband imaging? - Two Algorithms Urvashi Rau - Many Examples National Radio Astronomy Observatory Socorro, NM, USA 1/32

More information

STIS First Order Spectroscopic PSF s. Ted Gull, Don Lindler Nick Collins Don Tennant Bob S. Hill Eliot Malumuth

STIS First Order Spectroscopic PSF s. Ted Gull, Don Lindler Nick Collins Don Tennant Bob S. Hill Eliot Malumuth STIS First Order Spectroscopic PSF s Ted Gull, Don Lindler Nick Collins Don Tennant Bob S. Hill Eliot Malumuth Example: Eta Carinae Balmer Alpha 150 s Eta Carinae and Ejecta 52 x0.2 F1 (0.5 ) 10 s 0.3

More information

Swift XRT Data Analysis

Swift XRT Data Analysis Swift XRT Data Analysis Milvia Capalbi ASI Science Data Center (Frascati, Italy) Swift Team @ ASDC : P. Giommi, M.Capalbi,M.Perri (ASI - INAF) F.Tamburelli, B.Saija (Dataspazio) in collaboration with L.Angelini

More information

APO TripleSpecTool User s Guide

APO TripleSpecTool User s Guide APO TripleSpecTool User s Guide University of Virginia Astronomy Department July 16, 2009 Contents 1 Introduction 2 2 Installation 2 2.1 Computer Requirements....................................... 2 2.2

More information

Exoplanet transit, eclipse, and phase curve observations with JWST NIRCam. Tom Greene & John Stansberry JWST NIRCam transit meeting March 12, 2014

Exoplanet transit, eclipse, and phase curve observations with JWST NIRCam. Tom Greene & John Stansberry JWST NIRCam transit meeting March 12, 2014 Exoplanet transit, eclipse, and phase curve observations with JWST NIRCam Tom Greene & John Stansberry JWST NIRCam transit meeting March 12, 2014 1 Scope of Talk NIRCam overview Suggested transit modes

More information

GMT Instruments and AO. GMT Science Meeting - March

GMT Instruments and AO. GMT Science Meeting - March GMT Instruments and AO GMT Science Meeting - March 2008 1 Instrument Status Scientific priorities have been defined Emphasis on: Wide-field survey science (cosmology) High resolution spectroscopy (abundances,

More information

Paper Synopsis. Xiaoyin Zhu Nov 5, 2012 OPTI 521

Paper Synopsis. Xiaoyin Zhu Nov 5, 2012 OPTI 521 Paper Synopsis Xiaoyin Zhu Nov 5, 2012 OPTI 521 Paper: Active Optics and Wavefront Sensing at the Upgraded 6.5-meter MMT by T. E. Pickering, S. C. West, and D. G. Fabricant Abstract: This synopsis summarized

More information

erosita mirror calibration:

erosita mirror calibration: erosita mirror calibration: First measurements and future concept PANTER instrument chamber set-up for XMM mirror calibration: 12 m length, 3.5 m diameter: 8m to focal plane instrumentation now: f = 1.6

More information

An integral eld spectrograph for the 4-m European Solar Telescope

An integral eld spectrograph for the 4-m European Solar Telescope Mem. S.A.It. Vol. 84, 416 c SAIt 2013 Memorie della An integral eld spectrograph for the 4-m European Solar Telescope A. Calcines 1,2, M. Collados 1,2, and R. L. López 1 1 Instituto de Astrofísica de Canarias

More information

arxiv: v1 [astro-ph.im] 26 Mar 2012

arxiv: v1 [astro-ph.im] 26 Mar 2012 The image slicer for the Subaru Telescope High Dispersion Spectrograph arxiv:1203.5568v1 [astro-ph.im] 26 Mar 2012 Akito Tajitsu The Subaru Telescope, National Astronomical Observatory of Japan, 650 North

More information

Science Detectors for E-ELT Instruments. Mark Casali

Science Detectors for E-ELT Instruments. Mark Casali Science Detectors for E-ELT Instruments Mark Casali 1 The Telescope Nasmyth telescope with a segmented primary mirror. Novel 5 mirror design to include adaptive optics in the telescope. Classical 3mirror

More information

The 4mm (68-92 GHz) Receiver

The 4mm (68-92 GHz) Receiver Chapter 18 The 4mm (68-92 GHz) Receiver 18.1 Overview The 4 mm receiver ( W-band ) is a dual-beam, dual-polarization receiver which covers the frequency range of approximately 67-93 GHz. The performance

More information

arxiv: v1 [astro-ph.im] 23 Sep 2013

arxiv: v1 [astro-ph.im] 23 Sep 2013 CADRE: The CArma Data REduction pipeline D. N. Friedel a arxiv:1309.5844v1 [astro-ph.im] 23 Sep 2013 a University of Illinois, Department of Astronomy, 1002 W. Green St., Urbana, IL 61801 Abstract The

More information

WFC3 SMOV Program 11427: UVIS Channel Shutter Shading

WFC3 SMOV Program 11427: UVIS Channel Shutter Shading Instrument Science Report WFC3 2009-25 WFC3 SMOV Program 11427: UVIS Channel Shutter Shading B. Hilbert June 23, 2010 ABSTRACT A series of internal flat field images and standard star observations were

More information

Copyright 2002 by the Society of Photo-Optical Instrumentation Engineers.

Copyright 2002 by the Society of Photo-Optical Instrumentation Engineers. Copyright 22 by the Society of Photo-Optical Instrumentation Engineers. This paper was published in the proceedings of Optical Microlithography XV, SPIE Vol. 4691, pp. 98-16. It is made available as an

More information

Astro 500 A500/L-20 1

Astro 500 A500/L-20 1 Astro 500 1 Lecture Outline Spectroscopy from a 3D Perspective ü Basics of spectroscopy and spectrographs ü Fundamental challenges of sampling the data cube Approaches and example of available instruments

More information

ARRAY CONTROLLER REQUIREMENTS

ARRAY CONTROLLER REQUIREMENTS ARRAY CONTROLLER REQUIREMENTS TABLE OF CONTENTS 1 INTRODUCTION...3 1.1 QUANTUM EFFICIENCY (QE)...3 1.2 READ NOISE...3 1.3 DARK CURRENT...3 1.4 BIAS STABILITY...3 1.5 RESIDUAL IMAGE AND PERSISTENCE...4

More information

WISE Photometry (WPHOT)

WISE Photometry (WPHOT) WISE Photometry () Tom Jarrett & Ken Marsh ( IPAC/Caltech) WISE Science Data Center Review, April 4, 2008 TJ+KM - 1 Overview is designed to perform the source characterization (source position & flux measurements)

More information

APO TripleSpecTool User's Guide

APO TripleSpecTool User's Guide APO TripleSpecTool User's Guide Updated 09MAR2009 Table of Contents 7. APOTripleSpecTool 7.1. Installation 7.1.a. Computer Requirements 7.1.b. Download 7.1.c. IDL Setup 7.2. Data Preparation 7.3. Quickstart

More information

NASTER System Definition Proposal

NASTER System Definition Proposal Remote Sensing Team NASTER System Definition Proposal All rights reserved. - 7/14/03 Page 1 Overview Review and comment the mid-ir requirements Presentation of ABB s current platform technology Proposed

More information

Photometry, PSF Fitting, Astrometry. AST443, Lecture 8 Stanimir Metchev

Photometry, PSF Fitting, Astrometry. AST443, Lecture 8 Stanimir Metchev Photometry, PSF Fitting, Astrometry AST443, Lecture 8 Stanimir Metchev Administrative Project 2: finalized proposals due today Project 3: see at end due in class on Wed, Oct 14 Midterm: Monday, Oct 26

More information

Baseline Tests for the Advanced Camera for Surveys Astronomer s Proposal Tool Exposure Time Calculator

Baseline Tests for the Advanced Camera for Surveys Astronomer s Proposal Tool Exposure Time Calculator Baseline Tests for the Advanced Camera for Surveys Astronomer s Proposal Tool Exposure Time Calculator F. R. Boffi, R. C. Bohlin, D. F. McLean, C. M. Pavlovsky July 10, 2003 ABSTRACT The verification tests

More information

MEGARA FOCAL PLANE SUBSYSTEMS

MEGARA FOCAL PLANE SUBSYSTEMS MEGARA FOCAL PLANE SUBSYSTEMS Pérez-Calpena, A. 1, Arrillaga X. 2, Gil de Paz, A. 3, Sánchez-Blanco. E. 1, García-Vargas, M.L. 1, Carrera, M.A. 2, Gallego, J. 3, Carrasco E. 4, Sánchez, F.M. 5, Vílchez,

More information

To print higher-resolution math symbols, click the Hi-Res Fonts for Printing button on the jsmath control panel.

To print higher-resolution math symbols, click the Hi-Res Fonts for Printing button on the jsmath control panel. To print higher-resolution math symbols, click the Hi-Res Fonts for Printing button on the jsmath control panel. Radiometers Natural radio emission from the cosmic microwave background, discrete astronomical

More information

NGAO NGS WFS design review

NGAO NGS WFS design review NGAO NGS WFS design review Caltech Optical 1 st April2010 1 Presentation outline Requirements (including modes of operation and motion control) Introduction NGSWFS input feed (performance of the triplet

More information

Long-Range Adaptive Passive Imaging Through Turbulence

Long-Range Adaptive Passive Imaging Through Turbulence / APPROVED FOR PUBLIC RELEASE Long-Range Adaptive Passive Imaging Through Turbulence David Tofsted, with John Blowers, Joel Soto, Sean D Arcy, and Nathan Tofsted U.S. Army Research Laboratory RDRL-CIE-D

More information

German Receiver for Astronomy at THz Frequencies

German Receiver for Astronomy at THz Frequencies German Receiver for Astronomy at THz Frequencies ATM 1-5 THz, 14 km altitude German SOFIA workshop 28,02.2011 Page 1 GREAT - the Consortium GREAT, L#1 & L#2 channels PI-Instrument funded and developed

More information

Optical Imaging. (Some selected topics) Richard Hook ST-ECF/ESO

Optical Imaging. (Some selected topics)   Richard Hook ST-ECF/ESO Optical Imaging (Some selected topics) http://www.stecf.org/~rhook/neon/archive_garching2006.ppt Richard Hook ST-ECF/ESO 30th August 2006 NEON Archive School 1 Some Caveats & Warnings! I have selected

More information

to optical and charge diffusion effects

to optical and charge diffusion effects Instrument Science Report ACS 23-6 ACS WFC & HRC fielddependent PSF variations due to optical and charge diffusion effects John Krist June 25, 23 ABSTRACT The ACS point spread function remains fairly stable

More information

Master sky images for the WFC3 G102 and G141 grisms

Master sky images for the WFC3 G102 and G141 grisms Master sky images for the WFC3 G102 and G141 grisms M. Kümmel, H. Kuntschner, J. R. Walsh, H. Bushouse January 4, 2011 ABSTRACT We have constructed master sky images for the WFC3 near-infrared G102 and

More information

UM1380/ UM2380 UM1390/ UM2390 Datasheet

UM1380/ UM2380 UM1390/ UM2390 Datasheet UM1380/ UM2380 UM1390/ UM2390 Datasheet Description UM1380/ UM2380/ UM1390/ UM2390 spectro-module is a new OtO optical platform with 50% footprint down size compared to UM1280/UM2280 series. Besides the

More information

Imaging Simulations with CARMA-23

Imaging Simulations with CARMA-23 BIMA memo 101 - July 2004 Imaging Simulations with CARMA-23 M. C. H. Wright Radio Astronomy laboratory, University of California, Berkeley, CA, 94720 ABSTRACT We simulated imaging for the 23-antenna CARMA

More information

2 of this file: setenv SAS ODF *SUM.SAS 1 6. Now we can really procceed for obtaining the event lists. It usually takes several minutes, so type empro

2 of this file: setenv SAS ODF *SUM.SAS 1 6. Now we can really procceed for obtaining the event lists. It usually takes several minutes, so type empro How to work with XMM-Newton? Dmytro Iakubovskyi I. HOW TO START? To start working with XMM-Newton, please, open the terminal and go to your working direktory: cd /home/xmm DATA/guest/cenx3/. You will further

More information

The 20/20 telescope: Concept for a 30 m GSMT

The 20/20 telescope: Concept for a 30 m GSMT The : Concept for a 30 m GSMT Roger Angel, Warren Davison, Keith Hege, Phil Hinz, Buddy Martin, Steve Miller, Jose Sasian & Neville Woolf University of Arizona 1 The : combining the best of filled aperture

More information

Exoplanet Observing Using AstroImageJ

Exoplanet Observing Using AstroImageJ Exoplanet Observing Using AstroImageJ Dennis M. Conti Chair, AAVSO Exoplanet Section Copyright Dennis M. Conti 2017 1 AstroImageJ (AIJ) All-in-one freeware developed and maintained by Dr. Karen Collins

More information

Flux Calibration of the ACS CCD Cameras III. Sensitivity Changes over Time

Flux Calibration of the ACS CCD Cameras III. Sensitivity Changes over Time SPACE TELESCOPE SCIENCE INSTITUTE Operated for NASA by AURA Instrument Science Report ACS 2011-03 Flux Calibration of the ACS CCD Cameras III. Sensitivity Changes over Time Ralph C. Bohlin, Jennifer Mack,

More information

The Issues of Measurement of Optical Hazard Using Photometers EMRP JRP ENG05 Metrology for Solid State Lighting

The Issues of Measurement of Optical Hazard Using Photometers EMRP JRP ENG05 Metrology for Solid State Lighting The Issues of Measurement of Optical Hazard Using Photometers EMRP JRP ENG05 Metrology for Solid State Lighting Simon Hall,Paul Miller, Neil Haigh, Ben Thornton, Neil Haigh (Lux TSI) 25 th April 2013 Background

More information

Calibrating VISTA Data

Calibrating VISTA Data Calibrating VISTA Data IR Camera Astronomy Unit Queen Mary University of London Cambridge Astronomical Survey Unit, Institute of Astronomy, Cambridge Jim Emerson Simon Hodgkin, Peter Bunclark, Mike Irwin,

More information

OMEGA dataset. - 2 cubes (.QUB &.NAV) -1 software (readomega.pro under IDL)

OMEGA dataset. - 2 cubes (.QUB &.NAV) -1 software (readomega.pro under IDL) OMEGA dataset - 2 cubes (.QUB &.NAV) -1 software (readomega.pro under IDL) OMEGA DATA CUBE ORBNNNN_M.QUB sdat0 Idat S jdat sdat1 OMEGA GEOMETRY CUBE (ORBNNNN_M.NAV) geocube Bands 0-20: SWIR-C (All angles

More information

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan Southern African Large Telescope Prime Focus Imaging Spectrograph Instrument Acceptance Testing Plan Eric B. Burgh University of Wisconsin Document Number: SALT-3160AP0003 Revision 2.2 29 April 2004 1

More information

WFC3 TV2 Testing: UVIS Filtered Throughput

WFC3 TV2 Testing: UVIS Filtered Throughput WFC3 TV2 Testing: UVIS Filtered Throughput Thomas M. Brown Oct 25, 2007 ABSTRACT During the most recent WFC3 thermal vacuum (TV) testing campaign, several tests were executed to measure the UVIS channel

More information

A model for the SKA. Melvyn Wright. Radio Astronomy laboratory, University of California, Berkeley, CA, ABSTRACT

A model for the SKA. Melvyn Wright. Radio Astronomy laboratory, University of California, Berkeley, CA, ABSTRACT SKA memo 16. 21 March 2002 A model for the SKA Melvyn Wright Radio Astronomy laboratory, University of California, Berkeley, CA, 94720 ABSTRACT This memo reviews the strawman design for the SKA telescope.

More information

4DAD, a device to align angularly and laterally a high power laser using a conventional sighting telescope as metrology

4DAD, a device to align angularly and laterally a high power laser using a conventional sighting telescope as metrology 4DAD, a device to align angularly and laterally a high power laser using a conventional sighting telescope as metrology Christophe DUPUY, Thomas PFROMMER, Domenico BONACCINI CALIA European Southern Observatory,

More information

Week 10. Lab 3! Photometric quality. Stamp out those bad points. Finish it.

Week 10. Lab 3! Photometric quality. Stamp out those bad points. Finish it. Week 10 Lab 3! Photometric quality. Stamp out those bad points. Finish it. Lab 4! Great data. Evening sessions this week focus on Lab 3 wrap-up and Lab 4 reducgons. Exams ready for return Read the book!

More information

Camera 3 Intrapixel Sensitivity

Camera 3 Intrapixel Sensitivity Instrument Science Report NICMOS-99-005 Camera 3 Intrapixel Sensitivity A. Storrs, R. Hook, M. Stiavelli, C. Hanley, W. Freudling August 1999 ABSTRACT The NICMOS detectors have significant sensitivity

More information