Calibration Activities the MOS perspective
|
|
- Pauline Cooper
- 5 years ago
- Views:
Transcription
1 Calibration Activities the perspective Changing the Quantum Efficiency Calibration: Motivation and Justification.
2 Flux comparison using a sample (17) of AGN observations: as presented at MPE (May 2006) Band (kev) (1-PN)/PN (2-PN)/PN % +2.4% +6.8% +11.4% -1.6% +4.1% +7.3% +7.4%
3 v PN effective area discrepancy: 3C 273 comparison
4 Investigating additional transmission layers H2O 0.12 µm SiO Si3N Si 0.12
5 3C 273: What the PN sees Model: phabs*(po+po) N H = 1.79x10 20 cm -2 χ 2 = 1.08
6 Comparison: PN Model with 1 data and various QEs ICE 0.12 µm
7 Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO µm
8 Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO µm Si3N µm
9 Comparison: PN Model with 1 data and various QEs ICE 0.12 µm SiO µm Si3N µm Si 0.12 µm
10 Constraint on Si edge also precludes strong Si absorber Edge depth known Within ~2-3%
11 QE17 Adjustment of edges at C, N, O, only
12 Comparison with Orsay CCD1 1 CCD1 2
13 Comparison with Orsay CCD1 1
14 Model: phabs*(po+po) χ 2 = 1.19
15 All Const = 1.0 Model: const*phabs*(po+po): const(m1) = 1.03 const(m2) =1.06 χ 2 = 1.11 (with global renormalisation, c.f before without)
16 PN soft/hard slopes: Γ 1 =3.20(0.11) Γ 2 =1.63(0.01) M1 M2 qe16 M1 M2 qe17 Γ 1 =4.71(0.15) Γ 1 =4.65(0.15) Γ 1 =3.73(0.15) Γ 1 =3.76(0.15) Γ 2 =1.64(0.02) Γ 2 =1.69(0.02) Γ 2 =1.61(0.02) Γ 2 =1.65(0.02)
17 M1 M ES0102 M2 M
18 1 v RGS model, 1ES0102 Rev 0065 N H =5.36x10 20 cm -2 Const x (RGS model) kev 1 χ 2 = > 1.78 Const > χ 2 = > 2.30 Const > 0.90
19 1 v RGS model, 1ES0102 Rev 0981 N H =5.36x10 20 cm -2 Const x (RGS model) kev 1 χ 2 = > 2.16 Const > χ 2 = > 2.62 Const > 0.70
20 N H =5.36x10 20 cm -2 N H =8.00x10 20 cm -2
21 Zoom showing resolution adjustment required for later Revs
22 Comparison with Zeta Puppis On-axis Point Source Const x (RGS model) kev 1 χ 2 = > 1.49 Const > χ 2 = > 1.51 Const > 1.15
23 Independent astrophysical evidence? Spectral fitting to relatively high column density BL Lac N H ~ 4.4x10 20 cm -2 TBABS * PO Wilms abund kev 1 χ 2 = > χ 2 = > 1.08
24
25
26 (1-PN)/PN Thin Medium (2-PN)/PN
27 Problem with the psf? See talk by Andy later 3c 273: Flux Comparison, v extraction radii pn 1 2
28 Problem with the psf? See talk by Andy later MCG : 0, 7.5, 11.25, 15 inner extraction radii, 40 outer pn 1 2
29 Band (kev) (1-PN)/PN -5.4% +2.4% +6.8% +11.4% (2-PN)/PN -1.6% +4.1% +7.3% +7.4%
30
31 Quantum Efficiency measurements from Orsay 1 Central CCD
32 Quantum Efficiency measurements from Orsay 2 Central CCD
33 Surface Pixel Geometry in Monte Carlo model
34 SEM Pictures Side View Top View
35 (1-PN)/PN +12% +2%
36 (2-PN)/PN +12% +2%
37 H 2 O = 0.08 µm
38 H 2 O = 0.08 µm SiO 2 = 0.05 µm
39
40 Summary: Shape of the /PN discrepancy suggests problem lies with the quantum efficiency Adjustment of the QE would be consistent with Orsay measurements and probable uncertainties in model Adjusting the QE would leave a residual normalisation offset of about 5-7% between and PN Would need to increase global effective area or decrease PN global effective area to achieve absolute consistency low energy rmf would need re-calibration for consistency with any change in the QE
41 Comparison Count Rate/Effective of high energy Area portion normalised of the spectra to Rev from Datum and 903 Rate down 8% Eff. Area down 3% Flux down 5%
Status of the EPIC calibration
Status of the calibration 16 October 2003 Marcus G. F. Kirsch Marcus G. F. Kirsch with the input of the whole consortium Page 1 progress in calibration general absolute timing problem seems to be solved
More informationXMM-Newton Calibration
XMM-Newton Calibration Michael Smith, on behalf of XMM-SOC and Instrument Teams 18 th XMM-Newton Users Group Meeting, ESAC, 11 May 2017 ESA UNCLASSIFIED - For Official Use Outline 1. Status of calibration
More informationEPIC Straylight. telescopes/sieves/rga revisited. David Lumb, Athena Study Scientist
EPIC Straylight telescopes/sieves/rga revisited David Lumb, Athena Study Scientist Leicester BOC 7 Mar 2012 Topics Covered 1. The X-ray sieves 2. Initial in flight calibration (Crab ~Rev 54-56) 3. Sco
More informationXMM-Newton Chandra Blazar Flux Comparison. M.J.S. Smith (ESAC) & H. Marshall (MIT) 7 th IACHEC, Napa, March 2012
XMM-Newton Chandra Blazar Flux Comparison M.J.S. Smith (ESAC) & H. Marshall (MIT) 7 th IACHEC, Napa, March 2012 Blazar Sample Objective: Comparison of XMM-Newton Chandra fluxes in various bands. Using
More informationTemporal &Spatial Dependency of the MOS RMF
Temporal &Spatial Dependency of the RMF 1ES0102-72 1 Thin filter 0447 2 Thin filter 0447 0433 1ES0102 0.1-0.35 kev images Good spectra clean images Bad spectra bright patch - Able to do spectral analysis
More informationEvaluation of the capabilities of the XMM-Newton SciSim from the EPIC calibration point-of-view. André Burzlaff, FH Aachen
Evaluation of the capabilities of the XMM-Newton SciSim from the EPIC calibration point-of-view André Burzlaff, FH Aachen Menu XMM-Newton and EPIC SciSim Test Results Conclusion Outlook XMM Newton Launched
More informationENERGY SCALE IN EPIC-PN TIMING MODE
ENERGY SCALE IN EPIC-PN TIMING MODE Matteo Guainazzi1, Frank Haberl2, Michael Freyberg2, Michael Smith1 1 ESAC-ESA; 2MPE Outline What is the Timing Mode in EPIC-pn? Count rate dependence of the energy
More informationEPIC OBSERVATIONS OF BRIGHT BL LAC OBJECTS: WHAT CAN WE LEARN FROM THE X-RAY SPECTRA ABOUT THE ISM
1 EPIC OBSERVATIONS OF BRIGHT BL LAC OBJECTS: WHAT CAN WE LEARN FROM THE X-RAY SPECTRA ABOUT THE ISM F. Haberl 1, S. Sembay 2, B. Altieri 3, and W. Brinkmann 1 1 Max-Planck-Institut fu r extraterrestrische
More informationImproving the Relative Accuracy of the HETGS Effective Area
October 14, 2005 Improving the Relative Accuracy of the HETGS Effective Area Herman L. Marshall (MIT Kavli Institute) hermanm@space.mit.edu ABSTRACT I present updates to the HETGS grating efficiencies.
More informationJEREMY DRAKE, PETE RATZLAFF, VINAY KASHYAP AND THE MC CALIBRATION UNCERTAINTIES TEAM MONTE CARLO CONSTRAINTS ON INSTRUMENT CALIBRATION
JEREMY DRAKE, PETE RATZLAFF, VINAY KASHYAP AND THE MC CALIBRATION UNCERTAINTIES TEAM MONTE CARLO CONSTRAINTS ON INSTRUMENT CALIBRATION 11th IACHEC Meeting, Pune March 2016 JEREMY DRAKE, PETE RATZLAFF,
More informationPrincipal Component Analysis
Principal Component Analysis Revealing AGN Spectral Variability Michael Parker with Andy Fabian, Giorgio Matt, Erin Kara, Andrea Marinucci, Dom Walton, Karri Koljonen, Will Alston, Laura Brenneman and
More informationRGS CALIBRATION STATUS
RGS CALIBRATION STATUS ROSARIO GONZÁLEZ-RIESTRA XMM-NEWTON SCIENCE OPERATIONS CENTRE ON BEHALF OF THE SRON AND ESAC RGS TEAMS ESA UNCLASSIFIED - For Official Use Rosario Gonzalez-Riestra 17/05/2018 Slide
More informationMONTE CARLO METHODS FOR TREATING AND UNDERSTANDING HIGHLY-CORRELATED INSTRUMENT CALIBRATION UNCERTAINTIES
JEREMY DRAKE, PETE RATZLAFF, VINAY KASHYAP AND THE MC CALIBRATION UNCERTAINTIES TEAM MONTE CARLO METHODS FOR TREATING AND UNDERSTANDING HIGHLY-CORRELATED INSTRUMENT CALIBRATION UNCERTAINTIES Harvard Astrostatistics
More informationHigh Resolution X-Ray Spectra A DIAGNOSTIC TOOL OF THE HOT UNIVERSE
High Resolution X-Ray Spectra A DIAGNOSTIC TOOL OF THE HOT UNIVERSE Katarzyna Bensch Rosario González-Riestra María Santos-Lleó XMM-NEWTON / ESAC The RGS Instruments THE REFLECTION GRATING SPECTROMETER
More informationX-ray data analysis. Andrea Marinucci. Università degli Studi Roma Tre
X-ray data analysis Andrea Marinucci Università degli Studi Roma Tre marinucci@fis.uniroma3.it Goal of these lectures X-ray data analysis why? what? how? How? This is intentended to be a general reference
More informationChandra Analysis of a Possible Cooling Core Galaxy Cluster at z = 1.03
Chandra Analysis of a Possible Cooling Core Galaxy Cluster at z = 1.03 Kyle Dolan Institute for Astronomy, University of Hawaii at Manoa (Dated: 12 August 2005) We present an analysis of Chandra observations
More informationXMM-Newton Observations of the Isolated Neutron Star 1RXS J / RBS 1774
XMM-Newton Observations of the Isolated Neutron Star 1RXS J214303.7+065419 / RBS 1774 Mark Cropper, Silvia Zane Roberto Turolla Luca Zampieri Matteo Chieregato Jeremy Drake Aldo Treves MSSL/UCL Univ Padova
More informationRECONCILING PLANCK CLUSTER COUNTS AND COSMOLOGY?
RECONCILING PLANCK CLUSTER COUNTS AND COSMOLOGY? Chandra/XMM instrumental calibration and hydrostatic mass bias Holger Israel Durham University Birmingham Extragalactic Workshop 2015-02-17 HI, G. Schellenberger,
More informationAn explanation for the soft X-ray excess in AGN. Jamie Crummy collaborators: Andy Fabian, Luigi Gallo, Randy Ross Suzaku Team
An explanation for the soft X-ray excess in AGN Jamie Crummy collaborators: Andy Fabian, Luigi Gallo, Randy Ross Suzaku Team Soft excess The soft excess is at a constant temperature over a large range
More informationX-ray spectral Analysis
X-ray spectral Analysis xamples Problems Algorithm Model types Statistic Fitting procedure Practical problems with Chandra CCD data Disk N(N) Disk N(S) Nucleus Plume Based partly on the lecture given by
More informationCorrections for time-dependence of ACIS gain
Corrections for time-dependence of ACIS gain July 30, 2004 A.Vikhlinin,R.Edgar,N.Schulz Abstract There is a secular drift of the average PHA values for photons of a fixed energy E. This drift is caused
More informationBrandon C. Kelly (Harvard Smithsonian Center for Astrophysics)
Brandon C. Kelly (Harvard Smithsonian Center for Astrophysics) Probability quantifies randomness and uncertainty How do I estimate the normalization and logarithmic slope of a X ray continuum, assuming
More informationAthena Athena+ Towards a European Large X-ray Observatory. Mike Watson University of Leicester. Athena+
Athena Towards a European Large X-ray Observatory Mike Watson University of Leicester Topics Brief history and context New ESA approach to L-class selection The concept Credits: Athena & teams The road
More informationCalibration of the AGILE Gamma Ray Imaging Detector
Calibration of the AGILE Gamma Ray Imaging Detector Andrew Chen on behalf of the AGILE Team April 11, 2011 AGILE Astrorivelatore Gamma ad Immagini LEggero Italian Space Agency (ASI) small mission Participation
More informationThree data analysis problems
Three data analysis problems Andreas Zezas University of Crete CfA Two types of problems: Fitting Source Classification Fitting: complex datasets Fitting: complex datasets Maragoudakis et al. in prep.
More informationXMM-Newton SOC Technical Note
XMM-Newton SOC Technical Note XMM-SOC-CAL-TN-0082 Accuracy of energy reconstruction in EPIC-MOS Timing Mode M. Guainazzi April 6, 2009 History Version Date Editor Note 1.0 April 6, 2009 M.Guainazzi SASv8.0
More informationPerspectives on High Resolution X-ray Spectroscopy
Perspectives on High Resolution X-ray Spectroscopy Rewards and Challenges Claude R. Canizares MIT July 11-13, 2007 X-ray Spectroscopy Workshop Cambridge, MA Rewards of High Resolution X-ray Spectroscopy
More informationZeeman Effect. Alex Povilus Physics 441- Fall 2003 December 20, 2003
Zeeman Effect Alex Povilus Physics 441- Fall 2003 December 20, 2003 Abstract The Zeeman Effect is observed by application of a strong magnetic field to a mercury vapor cell and exciting transitions by
More informationSpectral Analysis of High Resolution X-ray Binary Data
Spectral Analysis of High Resolution X-ray Binary Data Michael Nowak, mnowak@space.mit.edu X-ray Astronomy School; Aug. 1-5, 2011 Introduction This exercise takes a look at X-ray binary observations using
More informationIntroduction Phase-Averaged Phase-Resolved Outlook PSR B Monitoring with RXTE from 1996 to Katja Pottschmidt (UCSD) May 2007
Monitoring with RXTE from 1996 to 2005 May 2007 S. Suchy (UCSD), J. Wilms (FAU), S. Haney (UCSB) R.E. Rothschild (UCSD) Source current RXTE-PCA PCU 2 rate, 3 20 kev top layer: 14.5 counts/s (Crab 1800
More informationCalibration of the IXPE Instrument
Calibration of the IXPE Instrument Fabio Muleri (INAF-IAPS) On behalf of the IXPE Italian Team 13th IACHEC Meeting 2018 Avigliano Umbro (Italy), 9-12 April 2018 IXPE MISSION IXPE will (re-)open the polarimetric
More informationCoronae of stars with supersolar elemental. abundances. Peretz 1 U., Behar 1 E., Drake 2 S.A. August 18, 2015
Peretz 1 U., Behar 1 E., Drake 2 S.A. 1 Department of Physics, Technion, Haifa 32000, Israel 2 USRA/CRESST & NASA/GSFC, Greenbelt, Maryland 20771, USA August 18, 2015 1 2 Spectra Main results FIP Bias
More informationCentral supermassive black holes from SINFONI observations
Central supermassive black holes from SINFONI observations R.P Saglia, MPE with R.Bender, N.Nowak, P. Erwin, J. Thomas Gas and stars in Galaxies A Multi-Wavelength 3D Perspective Garching, 10th June 2008
More informationA New Method for Characterizing Unresolved Point Sources: applications to Fermi Gamma-Ray Data
A New Method for Characterizing Unresolved Point Sources: applications to Fermi Gamma-Ray Data Ben Safdi Massachusetts Institute of Technology 2015 B.S., S. Lee, M. Lisanti, and B.S., S. Lee, M. Lisanti,
More informationModeling Compton Thick Obscuration in Accreting Supermassive Black Hole Systems
Modeling Compton Thick Obscuration in Accreting Supermassive Black Hole Systems Kendrah Murphy MIT Kavli Institute for Astrophysics & Space Research Tahir Yaqoob Johns Hopkins University/NASA GSFC Overview
More informationDetection of X-Rays. Solid state detectors Proportional counters Microcalorimeters Detector characteristics
Detection of X-Rays Solid state detectors Proportional counters Microcalorimeters Detector characteristics Solid State X-ray Detectors X-ray interacts in material to produce photoelectrons which are collected
More informationX-ray signatures of AGN outflows: multi-dimensional radiative transfer simulations
X-ray signatures of AGN outflows: multi-dimensional radiative transfer simulations Stuart Sim Knox Long (STScI) Lance Miller (Oxford) Daniel Proga (UNLV) T. Jane Turner (UMBC) James Reeves (Keele) Overview
More informationPoS(ICRC2017)765. Towards a 3D analysis in Cherenkov γ-ray astronomy
Towards a 3D analysis in Cherenkov γ-ray astronomy Jouvin L. 1, Deil C. 2, Donath A. 2, Kerszberg D. 3, Khelifi B. 1, Lemière A. 1, Terrier R. 1,. E-mail: lea.jouvin@apc.in2p3.fr 1 APC (UMR 7164, CNRS,
More informationVariable X-ray absorption in the mini-bal QSO PG
Variable X-ray absorption in the mini-bal QSO PG 1126-041 Margherita Giustini Massimo Cappi, George Chartas, Mauro Dadina, Mike Eracleous, Gabriele Ponti, Daniel Proga, Francesco Tombesi, Cristian Vignali,
More informationThe X-ray absorption in GRB afterglows
The X-ray absorption in GRB afterglows Darach Watson DARK Cosmology Centre Niels Bohr Institute University of Copenhagen Overview Downturn at low energies deviating from a power-law Very similar to photoelectric
More informationAccounting for Calibration Uncertainty in Spectral Analysis. David A. van Dyk
Bayesian Analysis of Accounting for in Spectral Analysis David A van Dyk Statistics Section, Imperial College London Joint work with Vinay Kashyap, Jin Xu, Alanna Connors, and Aneta Siegminowska ISIS May
More informationMonitoring The HRC-S UV Rate: Observations of Vega
Monitoring The HRC-S UV Rate: Observations of Vega Deron Pease, Vinay Kashyap, Jeremy Drake and Michael Juda 10 May 2005 Abstract We present an interim report on Chandra HRC-S calibration observations
More informationSynchrotron Radiation Representation in Phase Space
Cornell Laboratory for Accelerator-based ScienceS and Education () Synchrotron Radiation Representation in Phase Space Ivan Bazarov and Andrew Gasbarro phase space of coherent (left) and incoherent (right)
More informationMOLECULES IN THE CIRCUMNUCLEAR DISK OF THE GALACTIC CENTER
MOLECULES IN THE CIRCUMNUCLEAR DISK OF THE GALACTIC CENTER Implications from Chemical Modeling Nanase Harada 1, Denise Riquelme 1, Serena Viti 2, Karl Menten 1, Miguel Requena-Torres 1, Rolf Güsten 1,
More informationNuStar has similar area kev, Astro-H better at E> 80 Kev
NuStar has similar area 20-80 kev, Astro-H better at E> 80 Kev 10 3 1 HXI Effective Area [cm 2 ] 10 2 10 1 5 10 30 80 Energy [kev] NuStar and Astro-H HXI should have similar FOV HXI becomes background
More informationAccounting for Calibration Uncertainty in Spectral Analysis. David A. van Dyk
Accounting for in Spectral Analysis David A van Dyk Statistics Section, Imperial College London Joint work with Vinay Kashyap, Jin Xu, Alanna Connors, and Aneta Siegminowska IACHEC March 2013 David A van
More informationComets observed with XMM-Newton
A major step in cometary X-ray research Konrad Dennerl Max-Planck-Institut für extraterrestrische Physik Comets the most surprising X-ray objects in space 1996: Comet Hyakutake (C/1996 B2) EPIC Consortium
More informationThe Contribution of Active Galactic Nuclei to the Excess Cosmic Radio Background at 1.4 GHz
The Contribution of Active Galactic Nuclei to the Excess Cosmic Radio Background at 1.4 GHz David R. Ballantyne Center for Relativistic Astrophysics, School of Physics, Georgia Tech The Cosmic Backgrounds
More informationNIST DTSA-II ( Son of DTSA ): Step-by-Step
NIST DTSA-II ( Son of DTSA ): Step-by-Step Dale E. Newbury (grateful user) National Institute of Standards and Technology Gaithersburg, MD 20899-8370 NIST-NIH Desktop Spectrum Analyzer (DTSA) Spectral
More informationComputational Challenges from Imaging X-ray Polarimetry. Herman L. Marshall (MIT) and the IXPE Team
Computational Challenges from Imaging X-ray Polarimetry Herman L. Marshall (MIT) and the IXPE Team Outline Introduction to Polarimetry IXPE: the Imaging X-ray Polarization Explorer Computational Challenges
More informationDust formation in O-rich Miras and IK Tau
Dust formation in O-rich Miras and IK Tau David Gobrecht & Isabelle Cherchneff Basel University Colls.: Arkaprabha Sarangi & John Plane Why Galaxies Care About AGB Stars III Vienna 30 July 2014 Overview
More informationA precise census of compton-thick agn
A precise census of compton-thick agn using NUSTAR and SWIFT/BAT I. Georgantopoulos, A. Akylas Corral, A., Ranalli, A., LanZUISI, G. NATIONAL OBSERVATORY OF ATHENS outline Brief Introduction to Compton-thick
More informationX-ray Radiation, Absorption, and Scattering
X-ray Radiation, Absorption, and Scattering What we can learn from data depend on our understanding of various X-ray emission, scattering, and absorption processes. We will discuss some basic processes:
More informationX-ray reverberation: a tool to constrain the (evolving) disc geometry in BHXRBs
X-ray reverberation: a tool to constrain the (evolving) disc geometry in BHXRBs Barbara De Marco N. Copernicus Astronomical Center of the Polish Academy of Sciences In collaboration with: G. Ponti, P.O.
More informationX-ray Absorption Spectroscopy
X-ray Absorption Spectroscopy Nikki Truss November 26, 2012 Abstract In these experiments, some aspects of x-ray absorption spectroscopy were investigated. The x-ray spectrum of molybdenum was recorded
More informationXMM-NEWTON VIEW OF PKS : HARDNESS RATIO AND CROSS-CORRELATION ANALYSIS OF EPIC pn OBSERVATIONS
The Astrophysical Journal, 637:699 710, 2006 February 1 # 2006. The American Astronomical Society. All rights reserved. Printed in U.S.A. A XMM-NEWTON VIEW OF PKS 2155 304: HARDNESS RATIO AND CROSS-CORRELATION
More informationNuSTAR observation of the Arches cluster: X-ray spectrum extraction from a 2D image
NuSTAR observation of the Arches cluster: X-ray spectrum extraction from a 2D image Space Research Institute (IKI), Moscow, Russia E-mail: krivonos@iki.rssi.ru The NuSTAR mission performed a long (200
More informationDetection of Exoplanets Using the Transit Method
Detection of Exoplanets Using the Transit Method De nnis A fanase v, T h e Geo rg e W a s h i n g t o n Un i vers i t y, Washington, DC 20052 dennisafa@gwu.edu Abstract I conducted differential photometry
More informationSolar wind Magnetosphere Ionosphere Link Explorer: SoH X-ray Imager (SMILE-SXI)
Solar wind Magnetosphere Ionosphere Link Explorer: SoH X-ray Imager (SMILE-SXI) Steve Sembay SMILE-SXI PI Department of Physics and Astronomy University of Leicester, UK On behalf of the SMILE-SXI collaborabon
More informationHard X-ray AGN and the Cosmic X-ray Background
Hard X-ray AGN and the Cosmic X-ray Background Sergey Sazonov Space Research Institute, Moscow, Russia 1 Rome, Oct. 17, 2013 Plan Cosmic X-ray background: measurements, modeling and implications for heavily
More informationThe TV3 ground calibrations of the WFC3 NIR grisms
The TV3 ground calibrations of the WFC3 NIR grisms H. Kuntschner, H. Bushouse, J. R. Walsh, M. Kümmel July 10, 2008 ABSTRACT Based on thermal vacuum tests (TV3; March/April 2008), the performance of the
More informationSOME ASPECTS OF MONTE CARLO SIMULATION FOR EFFICIENCY CALIBRATION OF GERMANIUM DETECTORS
ICRM Gamma Spectrometry Workshop Paris, France 23-24 February 2009 SOME ASPECTS OF MONTE CARLO SIMULATION S.Hurtado Universidad de Sevilla SPAIN 1 MONTE CARLO SIMULATION DISADVANTAGES Self-absorption correction
More informationChandra Observation of Point Sources in the X-Ray Elliptical Galaxy NGC 1407
Chin. J. Astron. Astrophys. Vol. 4 (2004), No. 3, 221 230 ( http: /www.chjaa.org or http: /chjaa.bao.ac.cn ) Chinese Journal of Astronomy and Astrophysics Chandra Observation of Point Sources in the X-Ray
More informationThe perspectives of X-ray polarimetry on accreting sources
The perspectives of X-ray polarimetry on accreting sources (with MoCA: a Monte Carlo code for Comptonization in Astrophysics) FP7 Strong Gravity Project WP4 Comptonization models: spectra and polarization
More informationPart XI. Optimising Femtosecond K α Sources
Part XI Optimising K α Sources 333 / 353 K α sources Goals: maximize # photons < 100 fs pulse length minimize spot size (magnification) maximize throughput (ave. power) 334 / 353 Applications of femtosecond
More informationScintillation Detectors
Scintillation Detectors J.L. Tain Jose.Luis.Tain@ific.uv.es http://ific.uv.es/gamma/ Instituto de Física Corpuscular C.S.I.C - Univ. Valencia Scintillation detector: SCINTILLATION MATERIAL LIGHT-GUIDE
More informationChandra Source Catalog Energy Bands
Chandra Source Catalog Energy Bands Michael L. McCollough, CXC/SAO January 26, 2007 Abstract: Given below is the rational for deciding the energy bands and their associated effective energy (mono-energy
More informationConstraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background
Constraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background Fiorenza Donato @ Physics Dept., Un. Torino The gamma-ray sky - Minneapolis, October 10, 2013 Plan of my talk What
More informationUltra-fast disk wind from a high accretion rate black hole 1H
Ultra-fast disk wind from a high accretion rate black hole 1H 0707-495 Kouichi Hagino (ISAS/JAXA) H. Odaka, C. Done, R. Tomaru, S. Watanabe, T. Takahashi K. Hagino et al. 2016, MNRAS, 461, 3954 BREAKING
More informationAbsolute Flux Calibration for STIS First-Order, Low-Resolution Modes
Instrument Science Report STIS 97-14 Absolute Flux Calibration for STIS First-Order, Low-Resolution Modes Ralph Bohlin, Space Telescope Science Institute Nicholas Collins, Hughes STX/LASP/GSFC Anne Gonnella,
More informationCMOS Pixel Sensor for a Space Radiation Monitor with very low cost, power and mass. Outline:
CMOS Pixel Sensor for a Space Radiation Monitor with very low cost, power and mass Outline: Motivations & Specifications The first prototype design Perspectives Yang ZHOU, Jérome Baudot, Cyril Duverger,
More informationPACS Spectrometer Wavelength Calibration
PACS Spectrometer Wavelength Calibration H. Feuchtgruber Max-Planck-Institut für extraterrestrische Physik, Garching PACS WaveCal 1 Description of the Calibration Problem - Blue array: 400 pixels - Red
More informationExtended X- ray emission from PSR B /LS 2883 and other gamma- ray binaries
Extended X- ray emission from PSR B1259-63/LS 2883 and other gamma- ray binaries George Pavlov (Pennsylvania State University) Oleg Kargaltsev (George Washington University) Martin Durant (University of
More informationBright gamma-ray sources observed by DArk Matter Particle Explorer
Bright gamma-ray sources observed by DArk Matter Particle Explorer a, Kai-Kai Duan ab, Zhao-Qiang Shen ab, Zun-Lei Xu a, and Simone Garrappa c on behalf of the DAMPE collaboration a Key Laboratory of Dark
More informationThe first model was based only on the CANBERRA information which we. drawing. Canberra refused any other information.
Experimental and Monte Carlo determination of Gamma Spectrometry Efficiency Pavel Dryak, Petr Kovář Czech Metrology Institute February 2009 Leading motive of our testing The producer send the drawing after
More informationMAPPING THE INNERMOST REGIONS OF AGNS WITH SHORT TIMESCALE FE LINE VARIABILITY
1 MAPPING THE INNERMOST REGIONS OF AGNS WITH SHORT TIMESCALE FE LINE VARIABILITY Giovanni Miniutti, Kazushi Iwasawa, and Andrew C. Fabian Institute of Astronomy, Madingley Road, Cambridge CB3 0HA, UK ABSTRACT
More informationPSF in-flight calibration for MOS 1 and MOS 2 cameras
PSF in-flight calibration - MOS 1 - MOS 2 PSF in-flight calibration for MOS 1 and MOS 2 cameras Simona Ghizzardi Silvano Molendi PSF in-flight calibration - MOS 1 - MOS 2 OVERVIEW The data set The analysis
More informationQuantitative determination of the effect of the harmonic component in. monochromatised synchrotron X-ray beam experiments
Frascati Physics Series Vol. XXX (1997), pp. 000-000 Conference Title - Conference Town, Oct 3rd, 1996 Quantitative determination of the effect of the harmonic component in monochromatised synchrotron
More informationWinds and X-ray reverberation in AGN
Winds and X-ray reverberation in AGN Jane Turner (UMBC) James Reeves (Keele) Valentina Braito (Leicester) Andrew Lobban (Keele) Stuart Sim (MPA) Knox Long (STScI) Daniel Proga (Nevada) Steve Kraemer (Catholic)
More informationDust properties of galaxies at redshift z 5-6
Dust properties of galaxies at redshift z 5-6 Ivana Barisic 1, Supervisor: Dr. Peter L. Capak 2, and Co-supervisor: Dr. Andreas Faisst 2 1 Physics Department, University of Zagreb, Zagreb, Croatia 2 Infrared
More informationX-ray spectroscopy of nearby galactic nuclear regions
X-ray spectroscopy of nearby galactic nuclear regions 1. How intermittent are AGNs? 2. What about the silent majority of the SMBHs? 3. How do SMBHs interplay with their environments? Q. Daniel Wang University
More informationLecture Topics VMF Prof. Dr.-Ing. habil. Hermann Lödding Prof. Dr.-Ing. Wolfgang Hintze. PD Dr.-Ing. habil.
Lecture Topics. Introduction. Sensor Guides Robots / Machines 3. Motivation Model Calibration 4. 3D Video Metric (Geometrical Camera Model) 5. Grey Level Picture Processing for Position Measurement 6.
More informationObservational appearance of strong gravity in X-rays
Observational appearance of strong gravity in X-rays Compact object Companion star (5000 K) Schwarzschild radius Schwarzschild metric R s 2GM Schwarzschild radius (= 2.95 km for 1М ) c 2 Accretion Black
More informationCharacterization of low energy ionization signals from Compton scattering in a CCD Dark Matter detector
Characterization of low energy ionization signals from Compton scattering in a CCD Dark Matter detector Karthik Ramanathan University of Chicago arxiv:1706.06053 (Accepted PRD) TeVPA 2017/08/07 1 Motivation
More informationAC Fabian, M. Cappi, J Sanders. Cosmic Feedback from AGN
AC Fabian, M. Cappi, J Sanders Cosmic Feedback from AGN AC Fabian, M Cappi, J Sanders, S Heinz, E Churazov, B McNamara, J Croston, D Worrall, F Humphrey, F Tombesi, J Reeves, M Giustini, P O Brien, T Reiprich
More information1 Statistics Aneta Siemiginowska a chapter for X-ray Astronomy Handbook October 2008
1 Statistics Aneta Siemiginowska a chapter for X-ray Astronomy Handbook October 2008 1.1 Introduction Why do we need statistic? Wall and Jenkins (2003) give a good description of the scientific analysis
More informationX-ray Spectroscopy. Danny Bennett and Maeve Madigan. October 12, 2015
X-ray Spectroscopy Danny Bennett and Maeve Madigan October 12, 2015 Abstract Various X-ray spectra were obtained, and their properties were investigated. The characteristic peaks were identified for a
More informationNew Results of Fully Bayesian
UCI April 3, 2012 Calibration Samples Principle Component Analysis Model Building Three source parameter sampling schemes Simulation Quasar data sets Speed Up Pragmatic Bayesian Method Frequency Analysis
More informationThe Fast Spin of β Pic b
The Fast Spin of β Pic b! Jayne Birkby 1,2,* Ignas Snellen 2, Bernhard Brandl 2, Remco de Kok 2, Matteo Brogi 2, Henriette Schwarz 2 1 Harvard-Smithsonian Center for Astrophysics, USA; 2 Leiden Observatory,
More informationAbsolute energy calibration
E coeffs 1 Absolute energy calibration V. Morgunov DESY, Hamburg and ITEP, Moscow HCAL main meeting, DESY, January 19, 26 The copy of this talk one can find at the http://www.desy.de/ morgunov Jan 19,
More informationCharacterisation & Use of Array Spectrometers
Characterisation & Use of Array Spectrometers Mike Shaw, Optical Technologies & Scientific Computing Team, National Physical Laboratory, Teddington Middlesex, UK 1 Overview Basic design and features of
More informationAnalysis of extended sources with the EPIC cameras
Analysis of extended sources with the EPIC cameras 7 th ESAC SAS Workshop June 19 22, 2007 Science Operations Centre 1 Status Analysis of extended sources is complex, challenging and time-consuming There
More informationSolar cells operation
Solar cells operation photovoltaic effect light and dark V characteristics effect of intensity effect of temperature efficiency efficency losses reflection recombination carrier collection and quantum
More informationarxiv:astro-ph/ v2 12 Jan 2004
Astronomy & Astrophysics manuscript no. rxj0720 December 31, 2013 (DOI: will be inserted by hand later) Long-term variability in the X-ray emission of RX J0720.4-3125 Cor P. de Vries 1, Jacco Vink 1, Mariano
More informationScintillation Efficiency of Nuclear Recoils in Liquid Xenon. T. Wongjirad, L. Kastens, A. Manzur, K. Ni, and D.N. McKinsey Yale University
Scintillation Efficiency of Nuclear Recoils in Liquid Xenon T. Wongjirad, L. Kastens, A. Manzur, K. Ni, and D.N. McKinsey Yale University Scintillation Efficiency! By Definition: Ratio of light produced
More informationEXPOSURE TIME ESTIMATION
ASTR 511/O Connell Lec 12 1 EXPOSURE TIME ESTIMATION An essential part of planning any observation is to estimate the total exposure time needed to satisfy your scientific goal. General considerations
More informationDead Layer and Active Volume Determination for GERDA Phase II
Dead Layer and Active Volume Determination for GERDA Phase II Björn Lehnert on behalf of the GERDA Collaboration DPG Spring Meeting 05/02/2013 Dresden Institut für Kern- und Teilchenphysik Dead Layer (DL)
More informationXMM-Newton Calibration Technical Note
XMM-Newton Calibration Technical Note XMM-SOC-CAL-TN-0018 EPIC Status of Calibration and Data Analysis Edited by M.J.S. Smith (ESAC) on behalf of the EPIC Consortium December 12, 2016 History Version Date
More informationThe X-ray absorption in GRB afterglows
The X-ray absorption in GRB afterglows Darach Watson DARK Cosmology Centre Niels Bohr Institute University of Copenhagen Overview Downturn at low energies deviating from a power-law Very similar to photoelectric
More informationThe central region of M 31 observed with XMM-Newton
A&A 365, L195 L201 (2001) DOI: 10.1051/0004-6361:20000243 c ESO 2001 Astronomy & Astrophysics The central region of M 31 observed with XMM-Newton I. Group properties and diffuse emission R. Shirey 1,R.Soria
More information