L’ accrescimento sui buchi neri super massivi: la varieta' degli AGN … NHXM prospects L’ accrescimento sui buchi neri super massivi: la varieta' degli.

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Presentation transcript:

L’ accrescimento sui buchi neri super massivi: la varieta' degli AGN … NHXM prospects L’ accrescimento sui buchi neri super massivi: la varieta' degli AGN … NHXM prospects Roberto Maiolino (Oss. Roma) Guido Risaliti (Oss. Arcetri) Marco Salvati (Oss. Arcetri)

Emission components cold reflection power law FeK disk+corona circumnuclear “torus”

Cold absorbtion disk+corona obscuring “torus”

NHXM NuStar Red.  2 =1.01 No cut off! Continuum emission Disk + Corona model: Open questions: - Is the model correct ? (Comptonization spectra) - Geometry of the hot corona (Disc? Sphere?) - Electron temperature (  Cut-off energy) Componization Model: kT=100 keV Opt.depth=0.1

Continuum emission: low luminosity AGN Soft+Hard band: distinction between ADAF, reflection, photoionization De Cia et al reflection ADAF phot.

Absorption Detection of heavily obscured AGN (e.g. in ULIRGs) Suzaku NHXM Superantennae: (Braito et al. 09) Note: Even for AGN-dominated ULIRGs with N H ~10 24 cm -2, detection today possible only for ~3-5 objects!!

Absorption Absorption lines: wind/outflows in AGN: Requirements: High area in the 6-15 keV range to detect lines; Spectrum up to 100 keV to determine continuum NHXM NGC 1365 (Cappi et al. 2008) 1 st Case: Bright Seyferts, low-velocity outflows  physics of the gas Fe XXV K  Fe XXVI K  Fe XXV K  Fe XXVI K  V out ~ 3000 km/s

Absorption 2 nd Case: High-velocity outflows (feedback) in quasars

Absorption Variability: - Common (now seen in several Seyferts) - Powerful tool to study circumnuclear absorber - Need to consider it in any complete spectral analysis Risaliti et al. 2002,05,07,08,09 Elvis et al Puccetti et al Maiolino et al NGC 1365:  =30 ks  N H =2x10 23 cm -2  Cov.Fact.)=50% X-ray source cloud

Simulation with a realistic model: reflection, rel. line, soft exc., part. cov. 2 intervals, 10 ksec each. N H1 =2x10 23 cm -2, complete covering, N H2 =2x10 23 cm -2, Partial covering: CF1=40%  CF2=80% Absorption XMM: No C.F. variation NHXM: C.F. variation detected Cov. Fact. 1 Cov. Fact. 2

Absorption Compton thick partial covering: - Warped disk? - Very dense and very small clouds at the base of the disk driven wind? N H ~ cm -2 Cov. Fact ~ 80% transmitted component intrinsic component Only two cases known so far… …but may be much more common: their identification is limited by current sensitivities at E>10 keV (along with E <10 keV) Risaliti et al Turner et al. 2009

Reflection 1)Determination of continuum reflection component in bright AGNs -Currently uncertain by ~50% even in the brightest AGN -Needed to understand the structure & geometry of the circumnuclear medium cold reflection

Reflection 2) Study of reflection-dominated objects: Compton hump - Only NGC 1068 in bright catalogs (BAT, Integral) - Very few other spectra, NO ONE with good spectrum Awaki et al Energy (keV) NGC2273

Raban et al cos i keV keV keV Ghisellini et al mid-IR (dusty torus) Reflection 3) Reflection-dominated objects. Expected strong polarization: - energy-dependent: function of inclination angle wrt line of sight; - polarization angle: orientation of “reflector” on the sky  how does it compare with the other nuclear components? ionization cone

Probing Strong Gravity Probing GR effects in AGN spectra: 1)Iron (K, L) relativistic lines: shape & delays 2) Continuum polarization (NHXM): rotation of polarization angle Both methods provide independent measurements of the disk geometry and BH spin 1H Fabian et al Dovciak et al. 2004

“Old” XMM-Newton science -At least 3 times more 6 keV -Future of bigger mission uncertain (and very long time scales)  Broad Iron lines in bright objects (variability, profile)  Broad Iron lines in fainter objects (increasing the sample, are they ubiquitous?  Short time scale continuum variability (power spectra etc..)

Conclusions 1) High Energy spectra and X-ray polarimetry key to solve many outstanding open issues in AGN physics. 2) In many cases, soft (1-10 keV) + hard (>10 keV) needed to solve problems: hard spectra alone would not suffice. 3) More generally, the majority of AGN-related fields will enormously benefit of the unprecedented capabilities of NHXM  Key role as “observatory” available to the community (in contrast to PI missions such as NuStar)