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High Energy Astrophysics in the NexHigh Energy Astrophysics in the Next Decadet Decade
11June 2006June 2006
FromFrom INTEGRAL INTEGRAL toto SIMBOL-X SIMBOL-X
F. Lebrun
CEA-SaclaySAp/APC
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 22
INTEGRAL: a European gamma-ray observatoryINTEGRAL: a European gamma-ray observatory
SPI – The gamma-ray SPI – The gamma-ray Spectrometer of Spectrometer of INTEGRAL. Excellent INTEGRAL. Excellent spectra, good imagesspectra, good images
IBIS – The gamma-IBIS – The gamma-ray Imager onboard ray Imager onboard the INTEGRAL the INTEGRAL satellite. Excellent satellite. Excellent Imaging, good Imaging, good spectraspectra
ISGRIISGRI – the IBIS – the IBIS low energy low energy camera (CdTe)camera (CdTe) Perigee: 10,000 km,
Apogee: 150,000 km
Launch: October 2002
Operations funded Operations funded till end 2008till end 2008
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 33
511 keV bulge ~ 8°(Knödlseder et al., 2005)
1043 e+/s !Light dark matter ?
Point sources > 85%(Lebrun et al., 2004, Strong et al., 2005, Bouchet et al.,
2005)
Positronium ~ 92%(Jean et al., 2005
Weidenspointner et al., 2006)
60Fe(Harris et al., 2005)
26Al(Diehl et al., 2006)
GALACTIC DIFFUSE EMISSIONGALACTIC DIFFUSE EMISSION
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 44
• More than 200 sources detected with ISGRI More than 200 sources detected with ISGRI
(Bird et al., 2005)(Bird et al., 2005)
• 55 sources are new and heavily absorbed 55 sources are new and heavily absorbed
(N(NHH~ 10~ 102323 cm cm-2-2). ).
• HMXB population doubled HMXB population doubled
(mostly pulsar+supergiant companion)(mostly pulsar+supergiant companion)
• IGR J17456-290IGR J17456-290:: A steady non-thermal source near the GCA steady non-thermal source near the GC
• IGR J00291+5934IGR J00291+5934:: Fastest ms pulsar (P=1.67 ms), pulsed Fastest ms pulsar (P=1.67 ms), pulsed fraction increases with energyfraction increases with energy
• 4444Ti linesTi lines detected in the Cas A spectrumdetected in the Cas A spectrum
• MagnetarsMagnetars: very hard spectrum: very hard spectrum
POINT SOURCESPOINT SOURCES
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 55
Conclusions about ISGRI/CdTeConclusions about ISGRI/CdTe• No failure in 44 months of flight operationsNo failure in 44 months of flight operations• Noisy detectors: only 3%Noisy detectors: only 3%• PerformancesPerformances
– Sensitivity: milliCrab (3Sensitivity: milliCrab (3σ, tσ, tobsobs= = 1 day, 1 day, ΔE=E)ΔE=E)– Actual lower threshold: 15 keVActual lower threshold: 15 keV– Spectral performance is nominal Spectral performance is nominal
• 9% at 60 keV9% at 60 keV• 5% at 511 keV5% at 511 keV
– Spectral performance degradationSpectral performance degradation: : • ~ 2.6 % / year (factor 2 in 20 years)~ 2.6 % / year (factor 2 in 20 years)• 0.7 % after the November 2003 giant solar flare0.7 % after the November 2003 giant solar flare
CdTe/CdZnTe is confirmed as the X/gamma-ray CdTe/CdZnTe is confirmed as the X/gamma-ray detector for tomorrow space astrophysicsdetector for tomorrow space astrophysics
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 66
CNES calls for proposalsCNES calls for proposals
Selected for a phase A study (on-going)Selected for a phase A study (on-going)
• Micro satellites:Micro satellites: ECLAIRsECLAIRs
devoted to GRB study launch: 2011devoted to GRB study launch: 2011
• Formation flight:Formation flight: SIMBOL-XSIMBOL-X
Focusing hard X-rays launch: 2013Focusing hard X-rays launch: 2013
Final selection next yearFinal selection next year
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 77
Multiwavelength study of Multiwavelength study of Gamma-Ray Burst prompt emissionGamma-Ray Burst prompt emission
ECLAIRsECLAIRsFrance-ChinaFrance-China
SVOM payloadSVOM payload
Gamma-ray telescopeGamma-ray telescopeX-ray telescopeX-ray telescope
Optical telescopeOptical telescope
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 88
ECLAIRECLAIRSS: The X and Gamma Camera (CXG): The X and Gamma Camera (CXG)
Wide field of view (Wide field of view (~2 sr~2 sr) coded mask telescope encircled by a graded) coded mask telescope encircled by a graded
DetectDetectionion plane ( plane (DPIXDPIX) made of 200 XRDPIX modules developed) made of 200 XRDPIX modules developed
Array of CdTe Array of CdTe detectorsdetectors
XRDPIXXRDPIXmodulesmodules
Useful area 1024 Useful area 1024 cmcm22
Spectral band Spectral band 4.0 to 250 keV4.0 to 250 keV
100 GRB/year100 GRB/year40 cm40 cm
38 cm38 cm
52 cm52 cm
in the framework of CNES/CESR and CNES/CEA R&D programsin the framework of CNES/CESR and CNES/CEA R&D programs
shield collimator to reduce the cosmic diffuse induced backgroundshield collimator to reduce the cosmic diffuse induced background
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 99
CXG Anticipated PerformancesCXG Anticipated PerformancesC
ount
s
100
200
300
0
Energy (keV)10 40 605020 30
3.5 keV
The position on the sky of all The position on the sky of all GRBs detected with a signal to GRBs detected with a signal to
noise ratio greater than 5.5 will be noise ratio greater than 5.5 will be given with an accuracy given with an accuracy ~10′~10′
GRB 030227
20°
5h
Crab Nebula
INTEGRAL
Sen
sitiv
ity (
ph c
m-2 s
-1)
10
Peak energy (keV)100 100010
1
SWIFT
ECLAIRs
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1010
SIMBOL-XSIMBOL-X
0.5 – 80 keV0.5 – 80 keV
0.1–10 keV0.1–10 keV 15 keV-10 MeV15 keV-10 MeV
Focusing hard X-rays Focusing hard X-rays using formation flight technologyusing formation flight technology
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1111
Participating Participating laboratorieslaboratories
F : F : CEA/Saclay, CESR/Toulouse, APC/Paris, CEA/Saclay, CESR/Toulouse, APC/Paris, LAOG/Grenoble, Obs.Paris/MeudonLAOG/Grenoble, Obs.Paris/Meudon
It :It : (INAF :) O.A.Brera, Roma, Palermo, (INAF :) O.A.Brera, Roma, Palermo, IASF Milano, Bologna IASF Milano, Bologna
D : D : MPE Garching, I.A.A.TübingenMPE Garching, I.A.A.Tübingen
• End ‘01 :End ‘01 : First ideas & discussions CEA/Saclay & O.A.BreraFirst ideas & discussions CEA/Saclay & O.A.Brera• End ‘03 : End ‘03 : CNES call for ideas for formation flight…CNES call for ideas for formation flight…• Mid ‘04 : Mid ‘04 : Selection of 4 missions for an assessment phaseSelection of 4 missions for an assessment phase• End ‘05 :End ‘05 : Only Simbol-X is recommended for a phase A studyOnly Simbol-X is recommended for a phase A study
Short historyShort history
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1212
Simbol-X basicsSimbol-X basics
Focusing opticsCoded mask optics
Have the XMM angular resolution and sensitivity Have the XMM angular resolution and sensitivity in the INTEGRAL/ISGRI energy rangein the INTEGRAL/ISGRI energy range
INTEGRAL > 15 keV XMM < 10 keV
30 degrees30 degrees 30 arcmin30 arcmin
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1313
Major science goalsMajor science goals
Accreting Black HolesAccreting Black Holes
Physics in single objectsPhysics in single objects
Census in UniverseCensus in Universe
Particle Particle accelerationacceleration
Mechanisms ?Mechanisms ?
Maximum energy ?Maximum energy ?
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1414
• Record of Super Massive Black Record of Super Massive Black Holes accretion activityHoles accretion activity
•• Constraints to models for the Constraints to models for the formation and evolution of formation and evolution of structures in the Universestructures in the Universe
About 50 % resolved in sources in the 7–10 keV band
Accreting Black HolesAccreting Black HolesCensus of Super Massive Black HolesCensus of Super Massive Black Holes
But less than a few % resolved But less than a few % resolved beyond 10 keV, beyond 10 keV,
at the emission peak !at the emission peak !
CXB models : major contribution from CXB models : major contribution from obscured AGNs, but parametres are not obscured AGNs, but parametres are not constrained (evolution, energy cut-off, constrained (evolution, energy cut-off, absorption)absorption)
Need : resolve > 50 % of CXB in the [20-40] keV bandNeed : resolve > 50 % of CXB in the [20-40] keV band-> sensitivity, angular resolution, field of view-> sensitivity, angular resolution, field of view
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1515
Simbol-X : understand SgrA* and its environmentSimbol-X : understand SgrA* and its environment
Simbol–X, 300 ks,
> 10 keV 10x10 arcmin2XMM-Newton
INTEGRAL/IBIS/ISGRI
Simbol-X3 , 1 hour
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1616
Acceleration : link with HESS sourcesAcceleration : link with HESS sourcesprotons in SNRs shocks ?protons in SNRs shocks ?
G347.3-0.5 - HESS @ TeV
With Simbol-X :With Simbol-X :• • mapping of the synchrotron emission, mapping of the synchrotron emission, • • determination of spectral break with X-ray alone determination of spectral break with X-ray alone • • correlation with GeV and TeV emissionscorrelation with GeV and TeV emissions
SX
SN 1006SN 1006
Simbol-X : Simbol-X : E > 10 keVE > 10 keV
100 ks 100 ks 10’x15’10’x15’
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1717
Nucleosynthesis : measure Nucleosynthesis : measure 4444Ti yieldTi yield4444Ti : explosive nucleosynthesis product Ti : explosive nucleosynthesis product Period of 85 yearsPeriod of 85 yearsLines (Lines (4444Sc) at 68 and 78 keVSc) at 68 and 78 keV
Detected only in CasA (so far), by Detected only in CasA (so far), by BeppoSAX and INTEGRALBeppoSAX and INTEGRAL
10 a
rcm
in
100 ks
Map Cas A Map Cas A emissionemission
Simbol–X 44Ti map
Measure 1987A yieldMeasure 1987A yield
Spectrum 1 arcmin2
Measure Measure velocityvelocity
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1818
And a lot more…And a lot more…
• Quiescence : physical processes at low accretion rate, « ADAF », Quiescence : physical processes at low accretion rate, « ADAF », jets ?jets ?
• Difference between accreting neutron stars and black holes ?Difference between accreting neutron stars and black holes ?
• Follow and characterize the change of states on their evolutionary Follow and characterize the change of states on their evolutionary timestimes
• Local group population ?Local group population ?Absolute luminosity, localisationAbsolute luminosity, localisationhard X-ray spectrum : population characterization, comparison with hard X-ray spectrum : population characterization, comparison with Milky Way Milky Way
• Intermediate Mass Black Holes: ULXs characterization, spectrum Intermediate Mass Black Holes: ULXs characterization, spectrum and QPOs (and QPOs ( BH mass measurement) BH mass measurement)
• Cyclotron linesCyclotron lines
• Non thermal cluster emissionNon thermal cluster emission
• Young Stellar ObjectsYoung Stellar Objects
• Gamma-ray bursts follow upGamma-ray bursts follow up
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 1919
Simbol-X scientific requirementsSimbol-X scientific requirements
Energy band : Energy band : ~ 0.5 to > 80 ~ 0.5 to > 80 keVkeV
ΔΔE : < 150 eV @ 6 keV (Fe Ka)E : < 150 eV @ 6 keV (Fe Ka) < 1.3 keV @ 68 keV (< 1.3 keV @ 68 keV (4444Ti)Ti)
ΔΔ q : < 20 arcsec HPD q : < 20 arcsec HPD FOV : > 9 arcminFOV : > 9 arcminAttitude reconst. : ± 2 arcsecAttitude reconst. : ± 2 arcsec
ΔΔ t : < 100 microsecondest : < 100 microsecondes
Duration : 3 yearsDuration : 3 yearsOver 1000 targets possibleOver 1000 targets possible
Large effective area, excellent angular resolution, Large effective area, excellent angular resolution, very low backgroundvery low background
Sensitivity [1 Ms, 3 Sensitivity [1 Ms, 3 ] :] :1010-8-8 ph/cm ph/cm22/s/keV up to /s/keV up to ~ 80~ 80 keV keV1010-14-14 erg/cm erg/cm22/s [20-40 keV] (1 mCrab)/s [20-40 keV] (1 mCrab)
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2020
OpticsOptics
Focal length :Focal length : 20 - 30 m20 - 30 mShell diameters :Shell diameters : max 70 cmmax 70 cmShell thickness : 0.1 Shell thickness : 0.1 -- 0.3 mm 0.3 mmNumber of shells :Number of shells : ~ ~ 100100
• Heritage from XMM–Newton : nickel shells obtained by electroforming Heritage from XMM–Newton : nickel shells obtained by electroforming replication method; low mass obtained via a reduced thickness of shellsreplication method; low mass obtained via a reduced thickness of shells
• Coating : multi-layer Pt/C needed for requirement on large F.O.V. and on Coating : multi-layer Pt/C needed for requirement on large F.O.V. and on sensitivity up to > 80 keVsensitivity up to > 80 keV
Mirror parameters Mirror parameters to be optimized in phase Ato be optimized in phase A
Grazing incidence : Grazing incidence : Emax Emax 1/ 1/θθ Focal Length Focal Length
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2121
The focal detector assemblyThe focal detector assembly
Low energy detector (450 mm Silicon)Low energy detector (450 mm Silicon)(see L. Strüder talk on Friday)(see L. Strüder talk on Friday)
High energy detector (2 mm Cd(Zn)Te)High energy detector (2 mm Cd(Zn)Te)
Required parametRequired parameteersrs
• • Spectro-imaging system 0.5-100 keV Spectro-imaging system 0.5-100 keV
• • Pixel size ~ 500 mm (PSF oversampling)Pixel size ~ 500 mm (PSF oversampling)
• • Full size : 8x8 cm2, 128x128 pixelsFull size : 8x8 cm2, 128x128 pixels
• “• “Room temperature” operations (Room temperature” operations (~ -30°C)~ -30°C)
• • Fast reading (used in anticoincidence)Fast reading (used in anticoincidence)
Active anticoincidence shieldActive anticoincidence shield
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2222
Phase 0 result (CNES) : orbit pointing & stabilizationPhase 0 result (CNES) : orbit pointing & stabilization
20°
Sun
eclipticplane
sky area visible
at any moment 35%
360°
4,5 months
Transfer orbit
Increase of
perigee
orbital period
correction
High elliptical orbit : 44,000 - 256,000 km at launch
Orbit constraints : Orbit constraints : - have formation flight feasible (> - have formation flight feasible (> ~ 20,000 ~ 20,000 kkm)m)- minimize background (science > 75,000 km)- minimize background (science > 75,000 km)
Pointing : XMM / INTEGRAL typePointing : XMM / INTEGRAL typefixed solar panelsfixed solar panelssimplified thermal controlsimplified thermal control
Formation flight rFormation flight requirements : equirements : ± 10 cm along telescope axis± 10 cm along telescope axis± 1 cm perpendicular, knowldege @ ± 0.5 mm± 1 cm perpendicular, knowldege @ ± 0.5 mm
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2323
Phase 0 study (CNES) : detector spacecraft
COLLIMATOR
ISL back antenna
detectionradiatorand associatedheat pipe
lateralsensor
ISL antennas
fine SSTtowards -X
Detection payload
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2424
Phase 0 study (CNES) : mirror spacecraft
sun baffleISL back antenna
D=3m sky screen
thermal baffle
Wolter-I Mirror
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2525
Phase 0 study (CNES) : launch configuration
Launched as a composite under Soyuz
fairing
Masses
Detector S/C : ~ 600 kgMirror S/C : ~ 1300 kgAdapter : ~ 150 kg
Launcher capability :2.2 tons (5 deg incl.)
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2626
Status - scheduleStatus - schedule
• Simbol-X in phase A, conducted jointly by CNES & ASI, with the participation of MPE-IAAT
• Other partners are possible• End of phase A review : 2nd quarter 2007• Launch date : mid 2013
• Operations for three years (2 years of science observations)• Observation program will be composed of :
- a “core program”, with main priority science targets- and a guest observer program open to the community
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2727
Detector/Electronics requirementsDetector/Electronics requirements
• SIMBOL-X requirements:SIMBOL-X requirements:– Spatial resolution: 500 Spatial resolution: 500 μ μ small pixels small pixels– Spectral resolution: 1.3 keV @ 68 keV Spectral resolution: 1.3 keV @ 68 keV small pixels small pixels– Energy range: 10 – 100 keVEnergy range: 10 – 100 keV
• ECLAIRS CXG requirements:ECLAIRS CXG requirements:– Spatial resolution: 4 mmSpatial resolution: 4 mm– Energy range: 4 – 250 keVEnergy range: 4 – 250 keV
Front-end electronics :Front-end electronics :• - multi-channels ASIC / DC coupling - multi-channels ASIC / DC coupling • - Ultra low noise (< 40 e- RMS for stand alone chip)- Ultra low noise (< 40 e- RMS for stand alone chip)• - self triggered- self triggered• - Multiple event capabilities- Multiple event capabilities• - Low power, radiation tolerant, … as usual !- Low power, radiation tolerant, … as usual !
High Energy Astrophysics in the NexHigh Energy Astrophysics in the Next Decadet Decade
2828June 2006June 2006
High Energy DetectorArrays of Cd(Zn)Te with integrated ASICs
Tests of pixellatedCd(Zn)Te matrices
256 pixels CZT array 256 pixels CZT array 6 mm thick (eV-Products)6 mm thick (eV-Products)
256 pixels Schottky array 256 pixels Schottky array 0.5 mm thick (ACRORAD)0.5 mm thick (ACRORAD)
ASICs development (IDeF-X Vx.x)
Hybridization
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 2929
« Flat » prototype / CZT + IDeF-X V1.0« Flat » prototype / CZT + IDeF-X V1.0
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 3030
ISGRI : CdTe Pt/Pt : 4x4x2 mm3 / 120V / 0°C
5.6 keV FWHM2001
From ISGRI … 2001 to 2005From ISGRI … 2001 to 2005
ECLAIRS IDeF-X V1.0: CdTe In/Pt 4x4x1 mm3 / 600V / 24°C
1.8 keV FWHM2005
R&T IDeF-X V1.0 : CdTe In/Pt 2x2x0.5 mm3 / 340V / 24°C
1.1 keV FWHM(0.9 keV right side)0.73 keV FWHM
at 13.9 keV2005
June 2006June 2006 High Energy Astrophysics in the Next DecadeHigh Energy Astrophysics in the Next Decade 3131
ConclusionsConclusions• Current Results:Current Results:
• New low noise electronics under development for high resolution spectro-imaging New low noise electronics under development for high resolution spectro-imaging • 35 e35 e-- RMS achieved without detector RMS achieved without detector• 66 e66 e-- RMS achieved with a detector (330V, RT, dark current < 10 pA) RMS achieved with a detector (330V, RT, dark current < 10 pA)• « Flat » prototypes of 64 pixels 900µm, 1mm pitch used for evaluation and « Flat » prototypes of 64 pixels 900µm, 1mm pitch used for evaluation and
characterization of detector arrays characterization of detector arrays • CZT, CdTe and CdTe SchottkyCZT, CdTe and CdTe Schottky
• 0.5, 1 and 2 mm thick detectors are studied0.5, 1 and 2 mm thick detectors are studied
• 4 keV Low threshold value accessible with 4x4x1 Schottky detectors (600V / -4 keV Low threshold value accessible with 4x4x1 Schottky detectors (600V / -20°C) for the 20°C) for the ECLAIRsECLAIRs Mission Mission
• 1 keV FWHM at 60 keV accessible goal for 1 keV FWHM at 60 keV accessible goal for SIMBOL-XSIMBOL-X mission (small pixels) mission (small pixels)
• Current and next development steps :Current and next development steps :• New ASICsNew ASICs• Hybridization of ASICs and pixel arrays in progress Hybridization of ASICs and pixel arrays in progress • Space environment and Space qualification constraints studied simultaneously in Space environment and Space qualification constraints studied simultaneously in
the R&D programthe R&D program