D. E. McKenzie (Montana State University), S. Gburek (Space Research Centre, Polish Academy of Sciences), L. W. Acton, P. C. Martens (Montana State University)

Slides:



Advertisements
Similar presentations
RHESSI Investigations of the Neupert Effect in Solar Flares Brian R. Dennis AAS/SPD Meeting 6 June 2002.
Advertisements

On Estimation of Soil Moisture & Snow Properties with SAR Jiancheng Shi Institute for Computational Earth System Science University of California, Santa.
Evolving X-ray Polarimetry towards high energy and solar science Sergio Fabiani Università degli Studi di Roma “Tor Vergata” INAF / IAPS I A P S Istituto.
Basic Principles of X-ray Source Detection Or Who Stole All Our Photons?.....
RAPID-SCAN DOW RADAR OBSERVATIONS OF TORNADOES DURING VORTEX and 2010 Joshua Wurman, Karen Kosiba, Paul C. Robinson Center for Severe Weather Research.
Hard X-ray Production in a Failed Filament Eruption David, Alexander, Rui Liu and Holly R., Gilbert 2006 ApJ 653, L719 Related Paper: Ji. H. et al., 2003.
The Point Spread Function of the Yohkoh Soft X-ray Telescope D. E. McKenzie (Montana State University), S. Gburek (Space Research Centre, Polish Academy.
SPD/AAS Poster May 2007 Mark Weber Smithsonian Astrophysical Observatory On-Orbit Measurement of the Hinode / XRT Point Response Function.
Week 9 Presentation Brent Holmes. Yohkoh SXT I am using data from the Soft X- ray Telescope aboard Yohkoh.
White-Light Flares: TRACE and RHESSI Observations H. Hudson (UCB), J. Wolfson (LMSAL) & T. Metcalf (CORA)
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
RHESSI observations of LDE flares – extremely long persisting HXR sources Mrozek, T., Kołomański, S., Bąk-Stęślicka, U. Astronomical Institute University.
Measuring the Wilson effect: observations and modeling with RHESSI H. Jabran Zahid M. D. Fivian H. S. Hudson.
The First Adaptive Optics High Resolution Mid – IR Imaging of Evolved Stars: Case Studies of RV Boo and AC Her B.A. Biller, L.M.Close, D. Potter, J. Bieging,
Rocking Curve Imaging for Diamond Radiator Crystal Selection Guangliang Yang 1, Richard Jones 2, Franz Klein 3, Ken Finkelstein 4, and Ken Livingston 1.
Magnetic Reconnection Rate and Energy Release Rate Jeongwoo Lee 2008 April 1 NJIT/CSTR Seminar Day.
White-Light Flares via TRACE and RHESSI: Death to the thick target? H. Hudson, plus collaboration with J. Allred, I. Hannah, L. Fletcher, T. Metcalf, J.
Results Theory Abstract Evaluation of Scintillation Index and Intensity of Partially Coherent Laser Light MIDN 4/C Meredith L. Lipp and MIDN 4/C Kathryn.
EPIC Calibration Meeting, Madrid Correcting spatial inhomogeneities of the absolute energy scale K. Dennerl, 2010 March 23 Correcting spatial inhomogeneities.
O RBIS — Micro-EDXRF System. XRF Advantages Non-destructive: No beam damage or coating of sample Minimal Sample Preparation: conductivity not required.
EISCAT Tromsø. Progress in Interplanetary Scintillation Bill Coles, University of California at San Diego A. The Solar Wind: B. Radio Scattering: C. Observations:
NICMOS IntraPixel Sensitivity Chun Xu and Bahram Mobasher Space Telescope Science Institute Abstract We present here the new measurements of the NICMOS.
Grazing Incidence X-ray Scattering from Patterned Nanoscale Dot Arrays D.S. Eastwood, D. Atkinson, B.K. Tanner and T.P.A. Hase Nanoscale Science and Technology.
Rocking Curve Imaging for Diamond Radiator Crystal Selection Guangliang Yang 1, Richard Jones 2, Franz Klein 3, Ken Finkelstein 4, and Ken Livingston 1.
Apodized Filter IWA (λ/D)2~4 OWA (λ/D)13 Contrast ~10 -7 Throughput (%)41.4% Shape of the filter and the simulated coronagraphic point spread function.
Mineral grains from Ivuna ( ) Short summary 4 samples removed from the Ivuna meteorite were imaged at beamline BL47XU of SPring-8 on June 16,
Small scale magnetic energy release driven by supergranular flows Hugh Potts, Joe Khan and Declan Diver How to automatically detect and analyse supergranular.
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
Hard X and Gamma-ray Polarization: the ultimate dimension (ESA Cosmic Vision ) or the Compton Scattering polarimetery challenges Ezio Caroli,
Observations of Moreton waves with Solar-B NARUKAGE Noriyuki Department of Astronomy, Kyoto Univ / Kwasan and Hida Observatories M2 The 4 th Solar-B Science.
September 16, 2008LSST Camera F2F1 Camera Calibration Optical Configurations and Calculations Keith Bechtol Andy Scacco Allesandro Sonnenfeld.
NANO 225 Micro/NanoFabrication Electron Microscopes 1.
Solar space-born instruments and detectors for X-ray observations of the solar corona. Szymon Gburek Space Research Centre Polish Academy of Sciences,
Assessing Single Crystal Diamond Quality
Shapelets analysis of weak lensing surveys Joel Bergé (CEA Saclay) with Richard Massey (Caltech) Alexandre Refregier (CEA Saclay) Joel Bergé (CEA Saclay)
Development of CCDs for the SXI We have developed 2 different types of CCDs for the SXI in parallel.. *Advantage =>They are successfully employed for current.
Blind deconvolution of the SXT PSF core part Szymon Gburek Janusz Sylwester Space Research Centre, Polish Academy of Sciences Wrocław,Poland Multi-Wavelength.
Microscopia de Iones y Nano-Tecnología Eduardo H. Montoya Rossi.
The HESSI Imaging Process. How HESSI Images HESSI will make observations of the X-rays and gamma-rays emitted by solar flares in such a way that pictures.
Jyly 8, 2009, 3rd open meeting of Belle II collaboration, KEK1 Charles University Prague Zdeněk Doležal for the DEPFET beam test group 3rd Open Meeting.
14FEB2005/KWCAE2-UsersGroup Astro-E2 X-Ray Telescopes XRT Setup & Structure Performance Characteristics –Effective Area –Angular Resolution –Optical Axes.
The Helioseismic and Magnetic Imager (HMI) on NASA’s Solar Dynamics Observatory (SDO) has continuously measured the vector magnetic field, intensity, and.
Comparison b/w light and electron microscopes LIGHT MICROSCOPE ELECTRON MICROSCOPE Magnification can be done upto 2000 times Resolving power is less.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Index-matching effect. Matching the index of refraction of the bead with the solution.
U.A. Dyudina, A.P. Ingersoll, California Institute of Technology Pasadena, CA, Objectives We study lightning on Jupiter using spatially resolved.
Chromospheric Evershed flow
EVALUATION OF THE XMM NEWTON CROSS CALIBRATION ARCHIVE
Compact X-ray structures selection for determining SXT PSF shape
A Metallurgical Comparison of Mack T-12 Rod Bearings. Lots U, V & W
First Assessments of EUVI Performance on STEREO SECCHI
XRT Performance Update
Calibration of the Hinode X-ray Telescope (XRT)
Enlargements and area Scale factor Area of object Area of image.
Martin D Bootman, Michael J Berridge  Current Biology 
Statistical Deconvolution for Superresolution Fluorescence Microscopy
Efficient Receptive Field Tiling in Primate V1
Dongdong Li, Jun Xiong, Anlian Qu, Tao Xu  Biophysical Journal 
Image Restoration for Confocal Microscopy: Improving the Limits of Deconvolution, with Application to the Visualization of the Mammalian Hearing Organ 
A Map for Horizontal Disparity in Monkey V2
Singular Behavior of Slow Dynamics of Single Excitable Cells
Enlargement on Paper Enlarge the Rectangle by a Factor of 2
Soothing Massage of HMI Magnetic Field Data
Kinetics of Surface-Driven Self-Assembly and Fatigue-Induced Disassembly of a Virus- Based Nanocoating  Alejandro Valbuena, Mauricio G. Mateu  Biophysical.
Volume 111, Issue 4, Pages (August 2016)
Gaze and the Control of Foot Placement When Walking in Natural Terrain
Volume 84, Issue 3, Pages (March 2003)
Fig. 4 Pupil shape and image quality in the model sheep eye.
Diana L Pettit, Samuel S.-H Wang, Kyle R Gee, George J Augustine 
Efficient Receptive Field Tiling in Primate V1
106.13: A Makeover for HMI Magnetic Field Data
Presentation transcript:

D. E. McKenzie (Montana State University), S. Gburek (Space Research Centre, Polish Academy of Sciences), L. W. Acton, P. C. Martens (Montana State University) The Point Spread Function of the Yohkoh Soft X-ray Telescope Poster preparation for AAS meeting

Abstract The point spread function (PSF) of the Yohkoh solar observatory's Soft X-ray Telescope has two primary components, a sharply defined core and a diffuse wing due to photon scattering. Because the extent of the PSF is significantly wider than a single pixel, its characterization is useful for improvement of the quality of the SXT images. We will present results from analyses of the two PSF components, and demonstrate our best model of the core and scattering wing of the SXT point spread function. An example of PSF deconvolution to remove the effects of photon scattering will be given

Core part of the SXT PSF Properties: Size – about 5 pixels from the peak FWHM – approx. 1.5 pixels Depends on wavelength, position on the CCD

Calibration series to consider BX42_APR25 49 C K (0.28 keV/44.7 A) Best_Defoc XY Scan -> X,-11,500 to -2,500; Y, -6,500 to 2,500; Step 1,500 BX02_APR23 49 Al K (1.49 keV/8.34 A) Best_Defoc XY Scan -> X,-11,500 to -2,500; Y, -6,500 to 2,500 Step 1,500 BX51_APR25 49 Ag L (3.00 keV/4.16 A) Best_Defoc XY Scan -> X,-11,500 to -2,500; Y, -6,500 to 2,500; Step 1,500 Could be also BX21_APR24 49 C K Best_Defoc XY Scan -> X,-11,500 to -2,500; Y, -6,500 to 2,500; Step 1,500

bx42_apr25 calibration series

bx02_apr23 calibration series The image above shows 49 images of bx01_apr23 ground calibration series. Enlarged contour plots of their peak portions in the image bellow.

bx51_apr25 calibration series

Elipticity of the core calibration series bx42_apr25 bx02_apr23 bx51_apr25 The PSF core gets elliptically deformed with the distance from the CCD center. In the CCD corners can be even double peaked.

averaged core cross sections calibration series bx42_apr25 bx02_apr23 bx51_apr25 Solid line peak x-cross sections (upper row) and y-cross sections (the bottom row) for average PSF core for WSMR calibration series. The average PSF shape was determined from images 7-49 for each of (mentioned above) series respectively. Error bars show absolute errors for the selected images

Comparison of cross sections of averaged PSF core for different energies x-cross sections y-cross sections Al-K C-K Ag-L Al-K C-K Ag-L

Core aplications Aplications: Deconvolution of the SXT Flare images, mainly in horizontal belt shown to the left where eliptical deformation of the core PSF part is small. Above, a coverage map of the CCD detector surface by full resolution SXT frames. Gray intensity says how many times a given pixel was captured within a full resolution frame during year 2000.

SXT flare frame 8-MAY-00 at 10:50:21 Deconvolved image SXT flare frame (Log10 scale) Deconvolved image (Log10 scale) Example of deconvolution of SXT Flare images

PSF approximation from steepest descent method Calibration beam seen in Al.-K line Deconvolved PSF PSF cross sections (x-cross section in the left panel, to the right y-cross section. Thin solid line – cross sections of the PSF found by steepest descents method Thick solid line – cross sections of the calibration beam Diamonds – deconvolved PSF cross-sections