Gamma-Ray Observations Of
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Gamma-Ray Observations of SLAC Summer Institute, August 4th - August 15, 2008 Olaf Reimer Hansen Experimental Physics Labs & Kavli Institute for Particle Astrophysics and Cosmology, Stanford University AGILE first gamma-ray detection of a GRB: GRB 080514B (Mereghetti et al., to be submitted) SuperAGILE 1-D SuperAGILE – Mars Odyssey annulus GRB 080514B has been localized jointly by SuperAGILE and IPN (GCN 7715) and shows a significant gamma ray emission (GCN 7716). Follow-up by Swift (GCN 7719 and 7750) provided the afterglow in X-rays. Many telescopes participated in the observation of the optical afterglow: Watcher (GCN 7718), GRON (GCN 7722), KPNO (GCN 7725) and NOT (GCN 7734). Gamma-ray Observations of Supernova Remnants EGRET sources and Supernova Remnants A mixed blessing: • Spatial coincidences of UNIDs and cataloged (radio-)SNRs -23.0 2.00 W28 W44 -23.2 1.75 -23.4 1.50 Dec lination Dec lination -23.6 1.25 -23.8 1.00 270.4 270.2 270.0 269.8 269.6 284.75 284.50 284.25 284.00 R.A. R.A. γ Cyg 41.5 IC443 22.8 41.0 22.6 Declination Declination 40.5 22.4 40.0 Esposito et al. 1996 306.0 305.5 305.0 304.5 304.0 94.6 94.4 94.2 R.A. R.A. • No detections in cases like SN1006, Tycho & Kepler • multifrequency support, that several synchrotron nebulae in SNR harbour magnetospherically active neutron stars (i.e. CTA1) • GeV-measured gamma-ray source positions do not correlate well with X- ray bright rim/shell features (although hampered by angular resolution) • GeV-cutoffs already significant in EGRET-spectra → serious consideration of neutron star origin at GeV SNR-associations CTA1 W28 γCyg IC443 Zhang & Cheng 98 Cheng & Zhang 98 EGRET sources and Supernova Remnants – the X-ray view on the associations Cas A : central X-ray point source (Chakrabarty et al. 2001), unpulsed IC443 : X-ray point source + PWN outside EGRET contour (Olbert et al. 2001), hard point source (Keohane et al. 1997, Bykov& Bocchino 2001) γCyg: complete identification of EGRET GeV-contour (Brazier et al. 1996) → RX J2020.2+4026 However: Becker et al. 2005 CTA1: complete identification of EGRET GeV-contour (Brazier et al. 1998) → RX J0070.0+7302 W44: association with PSR 1853+01 + PWN (Harrus et al. 1997) W28: associaton with PSR 1801-23 ? 2EG J0008+73 / RX J0007.0+7302 2EG J2020+4026 / RX J2020.3+4026 G119.5+10.2 (CTA1) SNR G78.2+2.1 74o 00' 15' 41o 00' 30' 23°00' RX J2020.3+4026 HD 193322 AGN 45' ON I T A 30' o N 73 00' 30' I HD 229119 L C DECLINATION DE DECLINATION RX J0007.0+7302 15' 40o 00' 30' 22°00' 21°45' 30' 72o 00' hm hm hm hm hm hm 20 25 20 20 20 15 00 15 00 05 23 55 06h22m 20 18 16 RIGHT ASCENSION RIGHT ASCENSION RIGHT ASCENSION (2000) Nevertheless: statistical significant correlations with galactic objects found Montmerle et al. 1979 COS-B, SNRs, OBs → "SNOB" Sturner & Dermer 1995 EGRET, SNRs → significant positional correlation Esposito et al. 1996 EGRET, SNRs (X-ray) → 14 associations Romero et al. 1999 EGRET, SNRs (radio), OB, WR → 22 associations • overwhelming statistical evidence for SNR correlation • significant evidence for OB association correlation • marginal support for WRs and/or Of stars Torres, Romero et al. 2003 More than a single population of galactic γ-ray sources present in the EGRET data. SNR as prime candidate sources for Galactic Cosmic Rays TeV electrons – YES! → SN1006 as seen by ASCA (Koyama et al. 1995) But what about the hadrons? Evidence for hadronic particle acceleration in SNRs? “The spectrum is a good match to that predicted by pion decay, and cannot be explained by other mechanisms.” (Enomoto et al. 2002, Nature) IC interpretation in conflict with data ! π0 decay interpretation in conflict with data, too ! (Reimer & Pohl 2002) The steepness of previously measured spectrum not confirmed by HESS (Aharonian et al. 2004, 2006) And then there came H.E.S.S. – SNR seen by ground-based Cherenkov telescopes Supernova Remnants seen – primariy particle distribution > 100 TeV RX J1713.7-3946 as seen by H.E.S.S. RA SNR seen by 6:17 IC 443 MAGIC, VERITAS 8:52 RX J0852-4622 CANGAROO, HESS 14:42 RCW 86 HESS 17:13 RX J1713.7-3946 CANGAROO, HESS 18:00 W28 HESS 23:23 Cas A HEGRA, MAGIC, VERITAS Particles accelerated in shock On the scale of kyrs, Particles are fields decay / are confined to source damped and particles region by pre-existing diffuse out of the source or dynamically generated magnetic fields X-ray / gamma ray correlation Porter et al. (2006) Katz & Waxman (2007) Plaga (2007) electrons … H.E.S.S. X-rays ~ IC γ-rays B ~ 10 μG Key issue: protons + 10-4 electrons/proton Strenght of Berezkho & Völk (2006) magnetic + gas B ~ 100 μG field → B2 ~ ρ Lucek & Bell MNRAS 2000 Contour lines: ASCA X-rays + gas Y. Uchiyama et al. 2002 →πo →γ-rays ~ X-rays Where are we now with RXJ1713.7-3946? Archetypal SNR protons electrons – Close correlation with X-rays [+electrons] – Spectral shape [+protons] – IC interpretation implies (too) low B-field [+protons] – No tight correlation with molecular material [+electrons] • Not yet clear… – Need data at lower energies to be sure, e.g. GLAST H.E.S.S. Who will settle this quest? Simulated GeV-Spectrum of RXJ1713? Yes (in b/w perspective) GLAST GeV-Imaging of RXJ1713? GLAST Assumptions on 3EGJ1714 made, underlying: 5 year exposure, E > 3 GeV (Funk et al. 2006) If hadronic, do we see enough SNR, and at the right places? → GLAST The remaining freedom in the interpretation of VHE data will be constraint by E < 100 GeV data – and sensitive X-ray data (Uchiyama et al. 2007) (a) 3EGJ1714 will be refined/disentangled from RXJ1713. → Molecular Cloud interaction → improved (CfA & Nanten) CO surveys (b) GeV emission from RXJ1713 will be detected or an u.l. will be truly sensitive → sanity check for the leptonic models/hadronic models → SNR ACCELERATION SITE FOR HADRONS OR NOT ? (c) Nature of 1WGA J1713.4-3949 ? Compact object? Progenitor?? 1xx GeV to ~100 TeV – ground-based Cherenkov telescopes Non-morphological resolved SNR-detections: Cas A: HEGRA, MAGIC, VERITAS W28: HESS IC443: MAGIC, VERITAS ↓ shellsize < instumental resolution: unresolved ↓ The “composite” SNR/PWN: e.g. G0.0+0.1, HESS J1813, … Gamma-Rays from Pulsar Wind Nebulae Energy Flux Synchrotron π0 decay Inverse Compton Synchrotron: 2 Ex(keV) = 4 (B/1mG)(Ee/10TeV) Radio IR/Optical X-rays γ-rays VHE γ-rays IC (on CMB): 2 Eγ(TeV) ~ (0.05Ee) Energy Neutral pion decay: 〈Eγγ〉 ~ 0.15 Ep X-ray 10 keV X-ray → 10 TeV e- 1 TeV γ-ray → 20 TeV e- io d a → 6 TeV p γ R - ra y Synchrotron IC on target: Synch. (+CMB) Gamma-Rays from Pulsar Wind Nebulae The PWN Population • Many known X-ray PWN now identified as TeV emitters and almost all of the highest spin-down power radio pulsars have associated TeV emission – Efficient particle accelerators • May be easier to detect in TeV than keV ? – Integration over pulsar lifetime for TeV electrons (less cooling) – TeV instruments sensitive to more extended objects – no confusion with thermal emission – Many of our unidentified sources may be PWN H.E.S.S. sources near energetic pulsars 435 pulsars in HESS survey region* preliminary Implied efficiency Systematic studies Spin-down → TeV possible ! ~ 1% ATNF PSRs vs. TeV Carrigan et al. 2007 GeV vs. TeV Funk Reimer Torres Hinton 2008 random coinc. Spin-down energy flux in ergs/kpc2 HESS J1825-137 • PSR J1826-1334 – 3×1036 erg/s spin-down 4 HESS power, ~2× 10 years old • 5’ X-ray PWN – G 18.0-0.7 (Gaensler et al 2002) • 1° TeV γ-ray source – HESS J1825-137 (Aharonian et al 2005) – Energy dependent morphology • A first at TeV energies – Cooling of electrons away from pulsar? (t ∝ 1/E) cool [ 2 keV synchrotron emission comes from 200 TeV electrons (if B ≈ 10 μG)…, γ-rays come from lower energy electrons ] PWN (numerically) most prominent class of identified galactic γ-ray sources Archetypal (before HESS): Crab Now: diversity among the PWNs! • often extended, • displaced from PSR, • energy dependend morphology change Vela X Horns 2006 The binary system PSR B1259-63 / SS 2883 Periastron 7. March 2004 Be Star 10 M~ Discovery: H.E.S.S.,March 2004 First variable galactic TeV source. First in a new source class in HE g-rays. 48 ms Pulsar Complex interaction 3.4 y period between pulsar and star during periastron PSR B1259-63 Pulsar Johnston et al. 1992 Millisecond pulsar (T=48 ms) Mass of ca. 1.4 solar masses Massive Be-type companion star of ca. 10 solar masses Highly eccentric orbit (T= 3.4year) Massive star Shock front Closest impact is ~1013 cm or ~20 stellar radii Electron wind from a pulsar terminates onto the strong Be-star outflow Shocked electrons radiate in synchrotron (X-rays) & IC (TeV Gamma-rays) Very plausible scenario, theoretically predicted. -2 -1 Feb. 04 H.E.S.S. Flux >380 GeV [cm s ] The PSRB1259-63 fieldofview Periastron March 04 Apr./May 04 X-Ray Binaries as Gamma-Ray Sources Binary systems of a compact object (neutron star or black hole) and a stellar companion Matter is flowing over from the stellar companion onto the compact object. Angular momentum conservation => Formation of an accretion disk Matter in the accretion disk heats up to ~ 106 K => X-ray emission …more on X-Ray Binaries As in most accretion disk systems, this results in the formation of collimated outflows: Mildly relativistic jets: Γ ~ 2 Generally identified as radio jets X-ray binary spectra typically consist of a thermal disk component plus a hard power-law.