Spectral analysis on faint extended sources: problems and strategies. Gamma-ray Large Area Space Telescope Omar Tibolla Padova University DC2 Closeout.

Slides:



Advertisements
Similar presentations
GLAST Science Support CenterAugust 9, 2004 Overview of Analyzing GLAST Data David Band (GLAST SSC—GSFC/UMBC)
Advertisements

The Kavli FoundationThe National Science Foundation Unidentified EGRET Sources and the Extragalactic Gamma-Ray Background Vasiliki Pavlidou University.
The Kavli FoundationThe National Science Foundation Guaranteed Unresolved Point Source Emission and the Gamma-ray Background Vasiliki Pavlidou University.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #22.
Fermi-LAT Study of Cosmic-Ray Gradient in the Outer Galaxy --- Fermi-LAT view of the 3 rd Quadrant --- Tsunefumi Mizuno (Hiroshima Univ.), Luigi Tibaldo.
Simulating HESS SNRs Gamma-ray Large Area Space Telescope Omar Tibolla Padova University DC2 Closeout Workshop, Goddard Space Flight Center, 31 May – 2.
1Andrea Caliandro Search of Optimized Cuts for Pulsar Detection Andrea Caliandro - INFN Bari DC2 CloseOut May Goddard Space Flight Center.
GLAST Science Support CenterAugust 9, 2004 Likelihood Analysis of LAT Data James Chiang (GLAST SSC – SLAC)
Andrea Caliandro 1 Andrea Caliandro (INFN - Bari) on behalf the FERMI-LAT collaboration PSR J : the youngest gamma-ray pulsar in the Galaxy?
The 3rd Fermi Catalog arXiv: Zhang Xiao 2015/03/10.
1 Search for Dark Matter Galactic Satellites with Fermi-LAT Ping Wang KIPAC-SLAC, Stanford University Representing the Fermi LAT Collaboration.
GLAST LAT ProjectDC1 Closeout Workshop, Feb , Statistical Issues in Likelihood Analysis of LAT Data Seth Digel (HEPL/Stanford Univ.) & Guillaume.
SLAC, 7 October Multifrequency Strategies for the Identification of Gamma-Ray Sources Marcus Ziegler Santa Cruz Institute for Particle Physics Gamma-ray.
February 2004GLAST - DC1 Closeout Meeting GRB Detection & spectral analysis in DC1 Data Nicola Omodei Francesco Longo, Monica Brigida INFN Pisa.
T. Burnett: IRF status 30-Jan-061 DC2 IRF Status Meeting agenda, references at:
GLAST LAT Project 1S. Ritz GLAST Large Area Telescope: Data Challenge Overview December 2003 Steven Ritz Gamma-ray Large Area.
Pulsar modeling and simulations Gamma-ray Large Area Space Telescope Massimiliano Razzano Nicola Omodei LAT Collaboration Meeting (SLAC, August 29 th -
GLAST LAT Project 1S. Ritz Discussion: To Where From Here? DC1 Closeout Meeting February 13, 2004 S. Ritz Gamma-ray Large Area Space Telescope.
GLAST LAT ProjectDC1 Closeout Workshop, Feb , Post-DC1 Work Seth Digel (HEPL/Stanford Univ.) Post-DC1 Work.
Deterministic Modeling of the MOS Background Steve Snowden NASA/Goddard Space Flight Center EPIC Operations and Calibration Meeting Mallorca 1-3 February.
Source detection at Saclay Look for a fast method to find sources over the whole sky Provide list of positions, allowing to run maximum likelihood locally.
C&A 10April06 1 Point Source Detection and Localization Using the UW HealPixel database Toby Burnett University of Washington.
GLAST LAT Project 1S. Ritz DC1 Closeout Introduction February 2004 Steven Ritz Gamma-ray Large Area Space Telescope.
GLAST for Lunch 2004 Sept. 231 Fluctuation Analysis: Shadows of Invisible Sources What’s happening here?
GLAST LAT Project SLAC Jan. 12, 2004 Hammer-Aitoff map.
GLAST Science Support Center June 29, 2005Data Challenge II Software Workshop GRB Analysis David Band GSFC/UMBC.
The GLAST Mission Gamma-ray Large Area Space Telescope Omar Tibolla Padova University International School of Cosmic Ray Astrophysics, Erice (Italy) 20.
SLAC March 1 st 2006 GLAST LAT Software F.Longo GLAST LAT GLAST LAT SW Overview of Cookbook Examples Francesco Longo University and INFN, Trieste, Italy.
06/02/2006 M.Razzano - DC II Closeout Meeting Pulsars in DC2 preliminary results from an “optimized” analysis Gamma-ray Large Area Space Telescope Massimiliano.
Lecture 18 : Weighing the Universe, and the need for dark matter Recap – Constraints on the baryon density parameter  B The importance of measuring the.
Adam Zok Science Undergraduate Laboratory Internship Program August 14, 2008.
Julie McEnery1 Data Challenge II Logo by Stefano Ciprini.
Interaction of Cosmic-Rays with the Solar System Bodies as seen by Fermi LAT Monica Brigida Bari University For the Fermi LAT Collaboration.
Source catalog generation Aim: Build the LAT source catalog (1, 3, 5 years) Jean Ballet, CEA SaclayGSFC, 29 June 2005 Four main functions: Find unknown.
A Catalog of Candidate High-redshift Blazars for GLAST
Fermi LAT Monash University Nov 21, 2009 R.DuboisFermi LAT Science Analysis Tutorial1 Issues in a Nutshell LS5039 Low stats: 4k photons in 1 yr Strong.
Julie McEnery1 Data Challenge II. Julie McEnery2 Seth Digel, Diego Torres & Olaf Reimer on high-latitude molecular clouds, SNRs, XRBs, OB associations,
Observations of the Large Magellanic Cloud with Fermi Jürgen Knödlseder (Centre d’Etude Spatiale des Rayonnements) On behalf of the Fermi/LAT collaboration.
Flavour break-up July7th 2008 Our aim was modest: 1)To alter fc=0.15 to fc=0.09 following investigations of the charm fraction 2)To take into account the.
Fermi LAT Monash University Nov 21, 2009 R.DuboisFermi LAT Science Analysis Tutorial1 Things that can bite you: DIY cuts For Science Tools analysis, getting.
MARCH 11YPM 2015  ray from Galactic Center Tanmoy Mondal SRF PRL Dark Matter ?
TOWARDS THE FIRST FERMI SNR CATALOG F. Giordano 1, T. Brandt 2 & F. Acero 2, F. de Palma 1, J. Hewitt 2 for the Fermi Collaboration 1 University and INFN.
VERITAS Observations Of M 31 and some results about my recent work
GLAST LAT Project DC2 Closeout Workshop, GSFC, 31 May-2 June Comparisons of Searches for Sources in the DC2 Data S. W. Digel Stanford Linear Accelerator.
Diffuse Emission and Unidentified Sources
Status of pulsar simulation for DC 2 Gamma-ray Large Area Space Telescope Massimiliano Razzano Nicola Omodei GLAST DC2 Software Workshop (Goddard Space.
Source catalog generation for DC2 Aim (in order of priority): 1.Improve on source detection algorithm and error box. 2.Provide a list of source identifications.
GLAST LAT Project DC2 Software Workshop, GSFC, June 27-29, Analytical Objectives for Science Tools for DC2 for DC2 S. W. Digel Stanford Linear Accelerator.
Hiroyasu Tajima Stanford Linear Accelerator Center Kavli Institute for Particle Astrophysics and Cosmology October 26, 2006 GLAST lunch Particle Acceleration.
Status of pulsar simulation for DC 2 Gamma-ray Large Area Space Telescope Massimiliano Razzano Nicola Omodei GLAST DC II Software Workshop (Goddard Space.
GLAST Science Support Center November 8, 2005 GUC Action Item #15 AI#15: Pre-Launch GI Proposal Tools David Band (GSSC/JCA-UMBC)
Source catalog generation Aim: Build the LAT source catalog (1, 3, 5 years) Jean Ballet, CEA SaclaySLAC, 23 May 2005 Four main functions: Find unknown.
Likelihood analysis of small diffuse sources Riccardo Rando Elisa Mosconi, Omar Tibolla DC2 Kickoff Meeting – SLAC, 1-3 March 2006.
GAMMA RAY BINARIES WITH FERMI Chandreyee Maitra Crystal Nuansa Aini Harsha Raichur Partha Sarathi Pal Instructors Robin Corbet, Mariano Mendez.
Alessandro Buzzatti Università degli Studi di Torino / SLAC
Jean Ballet, CEA Saclay GSFC, 31 May 2006 All-sky source search
DC2 pulsars analysis: a population point-of-view
20 diffuse catalogue fans
with Xiang-Yu Wang, Ruo-Yu Liu, Fang-Kun Peng and P.H.T. Tam
EBL Absorption Signatures in DC2 Data
First day: Planets, Sun and Moon
Prospects for Observations of Microquasars with GLAST LAT
Optimizing Galaxy Simulations using FGST Observations
LAT performance for DC2 and the “4-panel plot”
Galactic Diffuse Emission for DC2
TRAINEE PRESENTATION The North and South Ecliptic Pole fields population Project supervisors: R. Saxton N. Loiseau Trainee student: Jaime Abella Payá.
10th ASTRI GENERAL MEETING
Bootstrap Segmentation Analysis and Expectation Maximization
Fermi LAT Observations of Galactic X-ray binaries
EBL Absorption Signatures in DC2 Data
Presentation transcript:

Spectral analysis on faint extended sources: problems and strategies. Gamma-ray Large Area Space Telescope Omar Tibolla Padova University DC2 Closeout Workshop, Goddard Space Flight Center, 31 May – 2 June 2006

Vela FoV Vela PSR RXJ (Vela Jr)?

Vela Jr? Is there really a source or is it only caused by Diffuse Galactic emission? Yes, it’s a source Is it extended? Is it Vela Jr? It seems so...

Vela Jr? (2) Yes, it is extended....and it seems also to have a structure...

Spectral analysis: directly Let’s consider a ROI centered in Vela Jr center ROI radius = 10 o. So at the same time we study all the 3 sources and the backgrounds directly.

Spectral analysis: directly (2) Vela PSR Galactic backgrounds Extragalactic background Residual components Using the LAT source catalog? No (Pulsars should have a Broken Power Law Spectrum)

Spectral analysis: directly (3) Vela PSR Galactic backgrounds Extragalactic background Residual components Freeing scale parameters? No The solution is trying to isolate sources and to study them separately... But the 3 sources are very close among them, so we must use small ROI, much smaller than LAT PSF. Cut in energy! (and more attention to higher energies gammas)

Another exemplum Extragalactic background Residual components Galactic backgrounds This exemplum is more impressive; letting free too much the parameters (in this case scale parameters), we can get also non physical solutions! So, after isolating sources and studying them separately...we should freeze their parameters as soon as possible...

Backgrounds ROI of radius = 2 o Centered in: RA = 138 o dec = o To know the backgrounds we consider a ROI near the sources we are studying but far enough to not be influenced by them = 2o

Backgrounds (2) Extragalactic background (fixed): constant diffuse emission Pref = 1.6 ( x ) Sp. Index= -2.1 Galactic backgrounds: modeled with MapCube file GP_gamma.fits The scale factor is almost 1 never change very much (up to ) Residual component: modeled with MapCube file residual.fits The scale factor is more than 3 times grater than we was expecting

PSR Now we try to isolate PSR ROI centered in the source: RA = o dec = o ROI radius = 2 o (remember that now the backgrounds are totally fixed)

PSR (2) So we ask python likelihood to fit PSR spectral behaviour with a Broken Power Law: Pref. = ( x ) Index 1 = Index 2= E B = Extragalactic background Residual components Galactic backgrounds But we don’t like this fit... in particular if we look the behaviour at higher energies... PSR

PSR (3) So we fix manually the Energy Break at 20 GeV and after we let that E B run up to 25 GeV... With E B = 20 GeV we obtain: Pref. = ( x ) Index 1 = Index 2= Residual components Extragalactic background Galactic backgrounds PSR with E B = 20 GeV

E B : 20 GeV  25 GeV PSR with E B = 25 GeV Galactic backgrounds Residual components Extragalactic background With E B = 25 GeV we obtain: Pref. = ( x ) Index 1 = Index 2= For E B : 20 GeV  25 GeV, results are very similar among them. (log L increase for E B  5 GeV... but for E B < 20 GeV the gap between model and experimental data becomes relevant... So we’ll use E B = 20 GeV ) PSR (4)

PSR Galactic backgrounds Residual components Extragalactic background We tried (with Luis Reyes) to use a single Power Law with an exponential cut-off: PSR (5) and the this curve fits much better, with the following parameters: Pref. = ( x ) Index = E B = P1= It looks much better…

Vela Now it’s Vela turn. ROI centered in the source: RA = o dec = o ROI radius = 2 o

Vela Galactic backgrounds Extragalactic background Residual components Vela Vela doesn’t create any problem. Its spectrum is fitted very well with a Broken Power Law: Pref. = ( x ) Index 1 = Index 2= E B = ( ) MeV

RXJ And what about Vela Jr model? We create a homogeneous disk fits file (MapSource)...and after we let that the radius of this circle runs from 1 o down to 0.8 o. Now we should know everything to face the study of RXJ So we go back to the ROI shown in slide 5 and we put in the model all the fixed parameters we have obtained until now...

Using the model Vela Jr (using a Single Power Low Spectrum hypothesis) with radius = 1 o, we obtain: Prefactor = ( x ) Spectral Index = RXJ (2) Vela PSR Residual components Galactic backgrounds Extragalactic background Note the 300% of uncertainity in the prefactor... In fact, we can’t see Vela Jr in the plot...and, all in all, even if the result would be correct, I don’t like it (in particular for this SNR...)... Something seems to be wrong...

Maybe having 2 source bright like Vela and PSR (almost one order of magnitude brighter than Vela Jr) make impossible the study of Vela Jr, amplifying too much its uncertainity.. PSR Galactic backgrounds Vela Extragalactic background Residual components Using the model Vela Jr with radius = 0.8 o, we obtain: Prefactor > ( + 2 ) ( x ) Spectral Index > -1 ( ) (Also in this case we can’t see Vela Jr in the plot...) There is really something wrong somewhere. We could try to simplify the problem... RXJ (3)

RXJ avoiding PSR In order to simplify the problem we could try to exclude PSR from the ROI. 2 reasons: -it’s impossible to exclude Vela -at higher energies it’s the only relevant source (so there we can hope to see traces of Vela Jr) ROI centered in : RA = 130 o dec = o ROI radius = 4.3 o

Galactic backgrounds Vela Residual components Extragalactic background PSR Vela Jr RXJ avoiding PSR (2) Using the model Vela Jr with radius = 1 o, we obtain: Prefactor = ( x ) Spectral Index = And I like this result... (Note that, even if PSR is not in the ROI, we should insert it in the model)

Galactic backgrounds Vela Vela Jr Extragalactic background Residual components PSR And finally let’s do the check moving the radius of the model of Vela Jr down to 0.8 o...both Prefactor and Spectral Index decrease slowly. With radius = 0.8 o we obtain: Prefactor = ( x ) Spectral Index = RXJ avoiding PSR (3) This seems to be the correct way to follow, but we should know much better the geometrical shape (or structure) of RXJ  OK

Galactic backgrounds Vela Vela Jr Extragalactic background Residual components PSR Let’s look if using the Power Law with the exponential cut-off for PSR , we’ll get some improvements; using for Vela Jr, radius = 1 o, we have: Prefactor = ( x ) Spectral Index = RXJ avoiding PSR (4) (The same results we obtained with the Broken Power Low; but we could expect it, excluding that Pulsar from the ROI)

Galactic backgrounds Vela Vela Jr Extragalactic background Residual components PSR For Vela Jr with radius = 0.8 o we obtain: Prefactor = ( x ) Spectral Index = again the same results we obtained before RXJ avoiding PSR (5) This seems to be the correct way to follow, but we should know much better the geometrical shape (or structure) of RXJ  OK

Next steps In the last slide we end saying that the next step should be, having a better spatial resolution of RXJ : 1- using better classes of gammas: using only gammas of class A could be very useful also for re-doing the spectral analysis we have just performed. 2- using higher cut in energy, in order to reduce the PSF 3- more detailed TS Maps 4- increase the observation time 5- try the new release of Science Tools (v7r2...here I used Science Tools v7r0p3) 6-in order to separate much better Vela and Vela Jr, it should be useful to have more cuts on CTB core (see Bill’s talk)

Acknowledgements In alphabetic order: -Bill Atwood; USFC, USA. - Giovanni Busetto; Padova University, Italy. - Seth Digel; SLAC, Stanford, USA. - Francesco Longo; Trieste University, Italy. - Elisa Mosconi; Padova University, Italy. - Riccardo Rando; Padova University, Italy. - Luis Reyes; GSFC, USA. - Francesca Maria Toma; Padova University, Italy.