GIS Data Processing. Eddie Breeveld MSSL/UCL

Similar documents
CORONAL DIAGNOSTIC SPECTROMETER SOHO CDS SOFTWARE NOTE No. 54 Version 2 August, SOHO CDS-GIS Instrument Guide

Relative intensity calibration of CDS-GIS detectors on SOHO using a plasma diagnostic technique

Estimating Magnetic Field Strength from the. TLRBSE Solar Spectra Data

Density Diagnostics for EIS

Physics 476LW Advanced Physics Laboratory Atomic Spectroscopy

Near Infrared Spectro-Polarimeter Use Case

AstroBITS: Open Cluster Project

IntelliCal FAQ Revised 9/27/12

Lab 4: Stellar Spectroscopy

Open Cluster Research Project

Developments & Limitations in GSR Analysis

Reduction procedure of long-slit optical spectra. Astrophysical observatory of Asiago

Understanding Your Spectra Module. Agilent OpenLAB CDS ChemStation Edition

Mimir NIR Spectroscopy Data Processing Cookbook V2.0 DPC

WFC3 IR Blobs, IR Sky Flats and the measured IR background levels

Alpha spectrometry systems. A users perspective. George Ham. 26 th May Date Month Year

FRAM V5.2. Plutonium and Uranium Isotopic Analysis Software

Watershed Modeling With DEMs

SUBJECT: SPIRE Spectrometer Detector Thermal Time Constant Derivation Procedure

Overlaying GRIB data over NOAA APT weather satellite images using OpenCPN

How to Make Photometric & Colorimetric Measurements of Light Sources using an Ocean Optics Spectrometer and SpectraSuite Software

Astro 3 Lab Exercise

Exercises for the 1st CASSDA school

2. To measure the emission lines in the hydrogen, helium and possibly other elemental spectra, and compare these to know values.

DOAS measurements of Atmospheric Species

SEAMLESS INTEGRATION OF MASS DETECTION INTO THE UV CHROMATOGRAPHIC WORKFLOW

DETERMINATION OF THE FORMATION TEMPERATURE OF Si IV IN THE SOLAR TRANSITION REGION

Simulations for H.E.S.S.

Wavelength Calibration Accuracy for the STIS CCD and MAMA Modes

Lab 6: Spectroscopy Due Monday, April 10

Machine Positioning Uncertainty with Laser Interferometer Feedback

Polar alignment in 5 steps based on the Sánchez Valente method

Report on the new EFOSC2 VPH grisms

arxiv:astro-ph/ v1 28 Jun 2002

NCS. New Control System for the 30m Telescope. TBD. 2005

Common questions when planning observations with DKIST Jan 30, 2018

The wavelength reconstruction from toroidal spectrometer image data

Exploring Data. Keck LRIS spectra. Handbook of CCD Astronomy by Steve Howell Chap. 4, parts of 6

Ground and On-Orbit Characterization and Calibration of the Geosynchronous Imaging Fourier Transform Spectrometer (GIFTS)

Satellite project, AST 1100

The Performance of the EUV Spectroscope (EXCEED) Onboard the SPRINT-A Mission

The IRS Flats. Spitzer Science Center

BOXA-II ON-STREAM X-RAY FLUORESCENCE ANALYZER. Technical Description Version 2 BGRIMM AUTOMATION

Calibration of the Modular Neutron Array (MoNA)

Solar UV Spectroscopy and Coronagraphy

THE MEASUREMENT OF SOLAR ULTRAVIOLET SPECTRAL IRRADIANCE PROBLEMS & SOLUTIONS

FIELD SPECTROMETER QUICK-START GUIDE FOR FIELD DATA COLLECTION (LAST UPDATED 23MAR2011)

Emission lines observed with Hinode/EIS

Background The power radiated by a black body of temperature T, is given by the Stefan-Boltzmann Law

YTÜ Mechanical Engineering Department

Calibration Routine. Store in HDD. Switch "Program Control" Ref 1/ Ref 2 Manual Automatic

PACS Wavelength Switching AOT release note

Experiment 4 Radiation in the Visible Spectrum

PACS Spectrometer Wavelength Calibration

Software BioScout-Calibrator June 2013

Improvement of Himawari-8 observation data quality

Astro 500 A500/L-15 1

Impacts of focus on aspects of STIS UV Spectroscopy

Solar Spectroscopy. with Hinode/EIS and IRIS. Magnus Woods With thanks to David Long UCL-Mullard Space Science Laboratory

REX Evaluation Guide. American Micro Detection Systems Inc March Lane, Suite 200 Stockton, CA 95219

1. Prepare the MALDI sample plate by spotting an angiotensin standard and the test sample(s).

BOWSER Balloon Observatory for Wavelength and Spectral Emission Readings

Delivery of a new ACS SBC throughput curve for Synphot

CHARA Meeting 2017 Pasadena, California

Agilent All Ions MS/MS

Fringe Correction for STIS Near-IR Long-Slit Spectra using Contemporaneous Tungsten Flat Fields

Flat Fields and Flux Calibrations for the COS FUV Channel at Lifetime Position 4

SBC FLATS: PRISM P-FLATS and IMAGING L-FLATS

Data Reduction - Optical / NIR Imaging. Chian-Chou Chen Ph319

Numerical processing of sunspot images using the digitized Royal Greenwich Observatory Archive

Objectives: (a) To understand how to display a spectral image both as an image and graphically.

Advanced Test Equipment Rentals ATEC (2832) Agilent 86130A BitAlyzer Error Analysis Getting Started

ICP-MS. High Resolution ICP-MS.

Overview of Hyperion On-Orbit Instrument Performance, Stability, and Artifacts

Building Inflation Tables and CER Libraries

Telescopio Nazionale Galileo. GIARPS mode. Short Observer s Guide. Prepared by Avet Harutyunyan

Updated flux calibration and fringe modelling for the ACS/WFC G800L grism

Lab VI Light Emitting Diodes ECE 476

Mnova Software for Analyzing Reaction Monitoring NMR Spectra

Spectral Analysis of High Resolution X-ray Binary Data

Angelika Dehn Rob Koopman 10 Years GOME on ERS-2 Workshop

ESPRIT Feature. Innovation with Integrity. Particle detection and chemical classification EDS

ACE Control System. 1.0-m Pomona College Telescope Table Mountain Observatory ACE User Manual April 2005 Revision All rights reserved.

Instrumentation, Observations and Data Analysis

Calibration of ACS Prism Slitless Spectroscopy Modes

Using Calibrated Specular Reflectance Standards for Absolute and Relative Reflectance Measurements

esac Release Note for the Herschel SPIRE Fourier-Transform Spectrometer Background Subtracted Spectra

REGISTAX (Paul Maxon s tutorial)

Determination of Nanoparticle Sizeand Number Concentration using the npquant Evaluation Module for Qtegra ISDS. The world leader in serving science

Nobeyama Radio Polarimeters (NoRP) Analysis Manual ver Nobeyama Radio Observatory, April 1, 2015

FLUORESCENCE APPLICATIONS

Standards-Based Quantification in DTSA-II Part II

Lab 4: Differential Photometry of an Extrasolar Planetary Transit

UV-Vis optical fiber assisted spectroscopy in thin films and solutions

Quantification of JEOL XPS Spectra from SpecSurf

Chemistry Department

Jasco V-670 absorption spectrometer

Menzel/Matarrese/Puca/Cimini/De Pasquale/Antonelli Lab 2 Ocean Properties inferred from MODIS data June 2006

LCO Global Telescope Network: Operations and policies for a time-domain facility. Todd Boroson

Transcription:

GIS Data Processing Eddie Breeveld MSSL/UCL erb@mssl.ucl.ac.uk

GIS Data Processing Introduction and status of the GIS system Planning GIS Observations Displaying GIS Data Correcting Instument Effects Fixed Patterning Ghosts Intensity Calibration GIS Data Processing 2

Background The GIS covers the wavelength ranges:150-220å, 255-340Å, 395-495Å and 655-785Å, with slits ranging from 2 2 to 8 50 and 4 240. The GIS has been working successfully for many years, the instrumental effects are now well understood. The detectors use MCPs and a novel, low power, position encoding system using spiral anodes (SPAN). Selected events from the MCPs are quantised using three 8-bit A-D converters, and a look up table to produce a 12- bit spectrum. Initial intensity and wavelength calibration come from the ground calibration performed at RAL before launch. The relative intensity calibration has been confirmed in-flight. GIS Data Processing 3

Current Status GIS Software User Manual and GIS Instrument Guide are published as CDS software notes. (http://orpheus.nascom.nasa.gov/cds/software_notes.html) Most areas of the GIS detectors are available for analysis. More than 2300 GIS rasters run, in over 1400 GIS observations, with 315 different GIS studies. Currently detector 2 is switched off because of a possible outgassing of insulating material since the recovery of SOHO. GIS Data Processing 4

Planning GIS Observations GIS is astigmatic - no spatial information from the spectrum: the slit and mirror can be moved to cover larger areas. GIS on-board data encoding is sensitive to count rates: the observer must specify a solar zone beforehand. These zones are: off limb, below 5 counts/second/pixel quiet sun, up to about 20 counts/second/pixel active region, over 20 counts/secound/pixel Combination of zone and slit defines which GIS setup (GSET) to use. GIS Data Processing 5

Displaying GIS data Access to GIS data is very similar to the NIS, i.e., using xcat, readcdsfits, etc. to read data into a quick look data structure (qlds). gis_plot can be used to display simple (average) plot of the data in a qlds. Images of two-dimensional data can be extracted from a qlds with gt_bimage, using the keywords lambda1 and lambda2 to select lines. mk_cds_map works as with NIS data, using the wrange keyword to select lines. GIS Data Processing 6

Correcting Instrument Effects The GIS has a number of instrument effects that need to be corrected for proper processing of the data. The use of a LUT introduces fixed patterning, not unusual with digital electronics. The SPAN encoders have an ambiguity in the spectral position of some of the incoming events. Intensity calibration and effective areas must be applied. GIS Data Processing 7

Fixed Patterning Seen in some parts of the detectors. Corrected with gis_smooth, which takes a qlds as input. GIS Data Processing 8

Ghosting Ghosts are displaced parts of spectral lines caused by an ambiguity of the encoding system. GIS Data Processing 9

Finding Ghosts - I First example, using the spectral line seen between 160 and 161Å. This line is in the ghosting regions defined by the bars on the plot. The theoretical quiet sun spectrum shows that there are no lines at this location. Further checking shows that the left shifted spectrum also has a line at this point. This strongly suggests that the line at about 160Å is a ghost. GIS Data Processing 10

Finding Ghosts - II Alternatively, if we are familiar with this area on the solar spectrum we know there is an FeXIII line at 202Å. To see whether this line needs correcting, first notice that it is a clear area of the plot, i.e., not in a ghosting area. Neither the left nor right shifted spectra show lines at this point, and thus this line is free from ghosts. The manual ghost correction software explains the process of moving the line in more detail, as well as overlaying a ghost cursor on the plot. GIS Data Processing 11

Ghost information files Used automatically by both the ghost plotting software and the ghost reduction software. Contain pixel location vs. expected ghosting for each GSET, and are included in the CDS SolarSoft directories. The information in these files comes from inspecting the raw files associated with each GSET. To read the contents of the ghost information file associated with a qlds and detector, use ghost_info. GIS Data Processing 12

Ghost Correction ghost_buster operates in two modes: Ghost Free: Removes all areas of the detectors that may contain ghosts. Manual: Allows the user the move ghosts back to the original locations See also http://www.mssl.ucl.ac.uk/www_solar/soho/gis_analysis.html GIS Data Processing 13

Ghost Free GIS Data Processing 14

Manual Ghost correction GIS Data Processing 15

Saving and Restoring Ghost Sessions By adding the save keyword to ghost_buster, it is possible to save the ghost corrections made in manual mode into an IDL structure variable. It is then possible to restore these corrections to uncorrected data with the restore keyword. GIS Data Processing 16

Wavelength Calibration Wavelength calibrations are automatic when the fits file is read in. The wavelength calibration can be accessed by the routines wave2pix and pix2wave, which translate the GIS pixel coordinates as necessary. Variations of about 20% of a line width are expected between observations, caused mainly by GIS hardware temperature differences when observing different parts of the sun, or very high count-rates causing distortions in the electronic processing. GIS Data Processing 17

Intensity Calibration Detectors and their electronics have non-linearities that need to be corrected. On the whole these corrections are less than 10%. gis_calib performs these corrections, with options to calibrate for the detector sensitivity and telescope effective area. The setmissing keyword can be used to mark parts of the data as missing if they cannot be calibrated. The region around the HeII 304Å line is so bright that the detector efficiency is less than 1% of the original efficiency; by default this region is also marked as missing. GIS Data Processing 18

Calibration details FIFO dead time: The dead time is a straightforward correction for an on-board First In First Out (FIFO) event queuing chip. Simple correction for Quiz-show dead time. Analogue dead time: This involves an extending dead time of approximately 2½ microseconds. Count rate dependant gain depression. Long term gain depression and flat field: Data files can be used to compensate for such gain depression. Detector / grating / telescope effective area. The calculations are based on the RAL pre-launch calibration exercise for the whole of CDS. GIS Data Processing 19

Using Calibrated Data - I Various CDS and other SolarSoft routines exist to use the data once calibrated; most of these can be used with both NIS and GIS data. The other utilities mentioned previously will also work with calibrated data. To extract the spectral data from a qlds always use utilities such as gt_windata or gt_spectrum; these routines will work with all storage schemes used for CDS data. GIS Data Processing 20

Using Calibrated Data - II Data returned from gt_windata are a floating point array of up to 4 dimensions: spectrum (always 2048 pixels for the GIS), solar x, solar y, and time. To get information about the extracted data use gt_windesc: The returned structure tells us which units the data use, the wavelength range, etc. Alternatively, xshow_struct can show all the information in the data structure. use gt_spectrum to get individual spectra from a raster. GIS Data Processing 21

Summary Can correct GIS data for detector effects. Ground calibration is used for sensitivity and effective area. GIS well used, but not as much as other SOHO instruments. GIS Data Processing 22

Further Work - I Confirm the in-flight absolute calibration. Quantify other detector effects (edge effects etc.) Implement automatic ghost correction where possible. Automate line profile fitting. GIS Data Processing 23

Further Work - II Read the GIS Instrument Guide and Software User Manual. Liaise with us with any GIS specific problems. Ask for more GIS observations. We would like feedback on any GIS related issue! GIS Data Processing 24

Some GIS results See http://www.mssl.ucl.ac.uk/~caf/firenze/firenze.html GIS Data Processing 25