NAM and UKSTP 11 April 2003 Sensitivity Differences in Pre-Loss and Post-Recovery NIS/CDS Spectrum By Steven Chapman Centre for Astrophysics University.

Slides:



Advertisements
Similar presentations
Estimating the Chromospheric Absorption of Transition Region Moss Emission Bart De Pontieu, Viggo H. Hansteen, Scott W. McIntosh, Spiros Patsourakos.
Advertisements

The Non-Flare Temperature and Emission Measure Observed by RHESSI J.McTiernan (SSL/UCB) J.Klimchuk (NRL)
ISSI, October 11-15, 2004 Synthesis of the Solar Spectrum including future plans Peter Fox HAO/NCAR Work partly funded by NSF/RISE and.
Coronal Boundaries of Active Regions Derived From Soft X-ray Images.
Measures of solar oblateness using active- region masking H.J. Zahid, M.D. Fivian, H.S. Hudson Space Sciences Lab, UC Berkeley.
The EUV spectral irradiance of the Sun from minimum to maximum Giulio Del Zanna Department of Space and Climate Physics University College London Vincenzo.
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
Ingolf E. Dammasch ROB/SIDC Brussels, Belgium Solar UV Spectroscopy with SUMER on SOHO (extended version for 11 Oct 2007)
The Non-Flare Temperature and Emission Measure Observed by RHESSI and SXI J.McTiernan (SSL/UCB) J.Klimchuk (NRL) Fall 2003 AGU Meeting.
08__050610_SCIP/SEB_PSR_Delivery.1 Temperature and Density Diagnostics with SECCHI EUVI J.S. Newmark Naval Research Laboratory (202)
Identifying and Modeling Coronal Holes Observed by SDO/AIA, STEREO /A and B Using HMI Synchronic Frames X. P. Zhao, J. T. Hoeksema, Y. Liu, P. H. Scherrer.
The Solar-B EUV Imaging Spectrometer: an Overview of EIS J. L. Culhane Mullard Space Science Laboratory University College London.
Coronal Holes Not As Well Behaved As We Thought Dustin Hickey Colby College ‘11 Montana State University Solar REU Program Advisor: Dana Longcope August.
Sunspot Studies in Oslo Nils Brynildsen, Per Maltby, Terje Fredvik and Olav Kjeldseth-Moe Institute of Theoretical Astrophysics University of Oslo.
Properties of Prominence Motions Observed in the UV T. A. Kucera (NASA/GSFC) E. Landi (Artep Inc, NRL)
Temperature Minimum Region between the Minimum-Activity Epochs and W. Livingston and E. Avrett AGU Fall Meeting, 2003.
1 Sunspot Studies in Oslo with CDS,SUMER,MDI and TRACE A final report (maybe). Per Maltby NilsBrynildsen Olav Kjeldseth-Moe, Per Maltby, Terje Fredvik.
CDS Session NAM Dublin April Active Region Loop Studies in Oslo Olav Kjeldseth-Moe and Terje Fredvik Institute of Theoretical Astrophysics University.
Andrzej Fludra Algorithm for automatic detection of coronal dimming as a tool for predicting CME’s Danielle Bewsher & Richard Harrison Presented by Andrzej.
A particularly obvious example of daily changing background noise level Constructing the BEST High-Resolution Synoptic Maps from MDI J.T. Hoeksema, Y.
Extracting the Mystery from the Red Rectangle Meghan Canning, Zoran Ninkov, and Robert Slawson Chester Carlson Center for Imaging Science Rochester Institute.
GIS – an update Dr Lucie Green Mullard Space Science Laboratory UCL.
This work utilizes data obtained by the Global Oscillation Network Group (GONG) Program and the SOI/MDI instrument on SoHO. GONG is managed by the National.
990901EIS_RR_Science.1 Science Investigation Goals and Instrument Requirements Dr. George A. Doschek EIS US Principal Investigator Naval Research Laboratory.
Analysis of Coronal Heating in Active Region Loops from Spatially Resolved TR emission Andrzej Fludra STFC Rutherford Appleton Laboratory 1.
Observing the Sun. Corona: EUV; X-rays Chromosphere: H , UV, EUV Photosphere: near UV, Visible light, infra-red.
Modeling the Solar EUV irradiance
First Results on Solar Irradiance Variability from PROBA2/LYRA/SWAP R. Kariyappa (guest investigator), S. T. Kumar, M. Dominique, D. Berghmans, L. Dame,
Variation of EUV solar irradiances along the cycle Vincenzo Andretta 1, Giulio Del Zanna 2, Seth Wieman 3 1 INAF – Osservatorio Astronomico di Capodimonte,
EUV Irradiance Reconstruction in view of PROBA2 Margit Haberreiter, PMOD/WRC, Davos, Switzerland Cis Verbeeck, Veronique Delouille, Rami Qahwaji ESWW9,
SOHO/CDS CDS Users’ Meeting, Sep 2005 Dr Peter Young, CCLRC/RAL Element Abundance Results from CDS Dr Peter Young Dr Peter Young SOHO/CDS Project Scientist.
High Resolution Imaging and EUV spectroscopy for RHESSI Microflares S. Berkebile-Stoiser 1, P. Gömöry 1,2, J. Rybák 2, A.M. Veronig 1, M. Temmer 1, P.
The Solar-B EUV Imaging Spectrometer: an Overview of EIS J. L. Culhane Mullard Space Science Laboratory University College London.
Locating the solar source of 13 April 2006 Magnetic Cloud K. Steed 1, C. J. Owen 1, L. K. Harra 1, L. M. Green 1, S. Dasso 2, A. P. Walsh 1, P. Démoulin.
Synchronic Magnetic Maps - the Inner Boundary Condition for the Heliosphere David Hathaway NASA Marshall Space Flight Center 2011 August 2 – Space Weather.
Standard DEM: Consider a imaging instrument with M EUV filters (for the EUVI Fe bands M = 3). The measured intensity in one image pixel is given by DEM.
Lecture 12 ASTR 111 – Section 002.
Comparison of Solar EUV Irradiance Measurements from CDS and TIMED/EGS W. T. Thompson L3 Communications EER, NASA GSFC P. Brekke ESA Space Science Department.
GOES fluence in Å and Å (1 min data) GOES fluence in Å and Å (1 min data) Areas in black correspond to times with the data missing.
CDS meeting September 2005 Solar Physics at UCLan Dr Barbara Bromage Centre for Astrophysics University of Central Lancashire.
Lessons Learnt from SOHO: CME Onsets CME Properties: to kg km/s Average span 45 o Significance: - Coronal evolution - Space weather.
CDS Users Meeting Sep In-flight monitoring and validation of the CDS NIS radiometric calibration Lang et al. Page 1 The in-flight monitoring.
Joint Planning of SOT/XRT/EIS Observations Outline of 90 Day Initial Observing Plans T. Shimizu, L Culhane.
DEVELOPING A SOLAR RADIOMETRIC CALIBRATION SYSTEM USING SPECTRAL SYNTHESIS. Peter Fox (HAO/NCAR) We present quantitative information on how we estimate.
GLOBAL ASYMMETRY OF THE SUN OBSERVED IN THE EXTREME ULTRAVIOLET RADIATION A. N. Zhukov ¹ ’ ², I. S. Veselovsky ², J.-F. Hochedez ¹, F. Clette ¹, O. A.
MOS Data Reduction Michael Balogh University of Durham.
Modeling the UV/EUV and its relevance for PROBA2 observations Margit Haberreiter Physikalisch-Meteorologisches Observatorium Davos/World Radiation Center,
Flare Prediction and the Background Corona Coronal Diagnostic Spectrometer Wolter-Schwarzschild Type 2 telescope Two separate spectrometers- the Normal.
Calculation of the Irradiance variations in the UV and extreme UV Margit Haberreiter PMOD/WRC, Davos, Switzerland IPC XI Sept 26 – Oct 15, 2010.
IMAGING AND SPECTOROPIC INVESTIGATIONS OF A SOLAR CORONAL WAVE: PROPERTIES OF THE WAVE FRONT AND ASSOCIATED ERUPTING MATERIAL L OUISE K. HARRA AND A LPHONSE.
Three-Dimensional Power Spectra of GONG++ High- Cadence Magnetograms F. Hill, J. Bolding, R. Clark, K. Donaldson-Hanna, J. Harvey, G. Petrie, C. Toner.
Sunspot activity and reversal of polar fields in the current cycle 24 A.V. Mordvinov 1, A.A. Pevtsov 2 1 Institute of Solar-Terrestrial Physics of SB RAS,
Calculation of the Coded Aperture zero-beam-size image (the “image”). The CA fitting procedure: The image is parameterized as a Sum-Of-Gaussians.
CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 20, 2005 Surface Magnetic Field Aschwanden, “Physics of the Solar Corona” Chap. 5, P.
Coronal Hole recognition by He 1083 nm imaging spectroscopy O. Malanushenko (NSO) and H.P.Jones (NASA's GSFC) Tucson, Arizona, USA Solar Image Recognition.
Solar & Heliospheric Observatory Rayana Thompson & Windell Barfield.
1 MURI:NADIR Progress on Area 6 solar features forecast October 2010.
GONG Measurements – Pre-eruptive signatures
VIRTIS flyby of Steins M-IR Spectral analysis
COS FUV Flat Fields and Signal-to-Noise Characteristics
VI. Forecasting Solar EUV/UV Radiation – EUV spectral synthesis
Carrington Rotation 2106 – Close-up of AR Mr 2106 Bt 2106
Exploring Large-scale Coronal Magnetic Field Over Extended Longitudes With EUVI EUVI B EIT EUVI A 23-Mar UT Nariaki Nitta, Marc DeRosa, Jean-Pierre.
First Assessments of EUVI Performance on STEREO SECCHI
W3 Preliminary Polarimetry Data
Studying Transition Region Phenomena with Solar-B/EIS
Magnetic connection between the photosphere and the corona
The Image The pixels in the image The mask The resulting image 255 X
Sushanta C. Tripathy NSO, Tucson
Presentation transcript:

NAM and UKSTP 11 April 2003 Sensitivity Differences in Pre-Loss and Post-Recovery NIS/CDS Spectrum By Steven Chapman Centre for Astrophysics University of Central Lancashire

NAM and UKSTP 11 April 2003 Contents Background on the side effects of the recovery of SoHO concerning CDS/NIS The Synoptic data Determining the modal low-emission intensity and showing the variation Aligning the pre-loss and post-recovery low-emission intensities Conclusion Aligning higher intensities

NAM and UKSTP 11 April 2003 Background… My main area of work has been studying the variation of the coronal hole area over cycle 23, with the CDS/NIS synoptic study. This will be combined with magnetic flux data to show how the open flux varies. This has involved contouring low-emission regions, but to do this you need a cut-off level between the low-emission region and the quiet sun.

NAM and UKSTP 11 April 2003 What Changed After the Recovery? The spectral line profiles of the NIS-1 and NIS-2 had acquired substantial wings on either side of the line. The sensitivity of the NIS-1 instrument has been noticeably reduced. NIS-2 sensitivity appears to be unaffected. CDS Software Note 53

NAM and UKSTP 11 April 2003 Pre-Loss and Post-Recovery Line profiles of Mg IX and Mg VII (NIS-1)

NAM and UKSTP 11 April 2003 Synoptic Data SoHO CDS Synoptic data is a long, near continuous data set. This is ideal to study changes in the behaviour of the CDS/NIS instrument Covers 5 lines in EUV wavelengths – He I, Fe XVI, Mg IX, Mg X (added in May 1998) and O V. The meridian of the Sun is covered by 9 rasters. Each raster is a cube of data. A 2D image where each pixel is made up of a spectrum of the mentioned lines.

NAM and UKSTP 11 April May EIT 195Å Full Disk of the Sun, with CDS synoptic pointings of all nine rasters overlaid

NAM and UKSTP 11 April May 1998 Mg IX Meridian Strip IntensityContoured Low-Emission Extracted Low-Emission

NAM and UKSTP 11 April 2003 Finding the Modal Low-Emission Intensity Histograms of all the masked pixels intensities are created. The peak shows the most common low-emission intensity for each masked image.

NAM and UKSTP 11 April 2003 Variation of the Modal Low-Emission Intensity, Uncorrected

NAM and UKSTP 11 April 2003 Aligning the Post-Recovery Low-Emission Intensities, Correction = 1.45

NAM and UKSTP 11 April 2003 Aligning the Post-Recovery Low-Emission Intensities, Correction = 1.8

NAM and UKSTP 11 April 2003 Aligning the Post-Recovery Low-Emission Intensities, Correction = 2.2

NAM and UKSTP 11 April 2003 Conclusion The sensitivity of the NIS1 instrument has been affected by the temporary loss of SoHO. The post-recovery low-emission intensities need a correction factor of ~1.8 to align it with the pre-loss. This investigation has only been done with ~300 days of data. Work is currently being done in studying all of the CDS synoptic data, to determine an acceptable low-emission correction factor for post-recovery NIS-1 data.

NAM and UKSTP 11 April 2003 Preliminary Investigation into Other Intensity Levels Early results in aligning post-recovery to pre-loss intensity levels shows that a non-constant correction factor is needed. Masked images have been created with a Mg X image using the following intensity level bands. These have been overlaid with the corresponding Mg IX image and then the pre and post intensity levels have been aligned (Coronal Hole) (Quiet Sun) ∞ (Active Region) (intensity units – photons-events/sec/pixel)

NAM and UKSTP 11 April 2003 A Non-Constant Correction Factor