A pulsar wind nebula associated with PSR J as the powering source of TeV J
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1 A pulsar wind nebula associated with PSR J as the powering source of TeV J Javier Moldón Netherlands Institute for Radio Astronomy Extreme Astrophysics in an Ever-Changing Universe Crete, June 16, 2014
2 Collaborators J. M. Paredes, Universitat de Barcelona V. Zabalza, The University of Leicester V. Bosch-Ramon, Universitat de Barcelona M. Ribó, Universitat de Barcelona J. Martí, Universidad de Jaén M. Kramer, Max-Planck-Institut für Radioastronomie A. G. Lyne, Jodrell Bank Centre for Astrophysics, The University of Manchester B. W. Stappers, Jodrell Bank Centre for Astrophysics, The University of Manchester Extreme Astrophysics Collaborators 2
3 The gamma-ray sky VHE (> 100 GeV) sky as seen by Cherenkov telescopes. 140 sources 46 extragalactic. 61 galactic. 30 unidentified Extreme Astrophysics Introduction 3
4 First unidentified source: TeV J Observed by HEGRA in Significance of 6.1σ Steady flux on yr timescales Extended with radius 6.2 ± 1.2 ± 0.9 arcmin Hard spectrum with index 1.9 ± 0.1 stat ± 0.3 /rmsys Integral flux > 1 TeV at the level of 5% Crab [Aharonian et al. 2002, A&A 293, L37] Extreme Astrophysics Introduction 4
5 TeV counterpart (MAGIC) [Albert et al. 2008, ApJ, 675, L25] Extension of the energy spectrum down to 400 GeV. No spectral break Extension of the source: 5 arcmin (assuming Gaussian shape) No flux variability over several yr, compatible with HEGRA (not Whipple) Extreme Astrophysics Introduction 5
6 TeV counterpart (VERITAS) [Aliu et al. 2014, ApJ 783, 16] Extreme Astrophysics Introduction 6
7 PSR J [Camilo et al. 2009, ApJ 705,1] Fermi: GeV pulsar LAT PSR J [Abdo et al. 2009, Sci 325, 840] P = 143 ms, τ c = 0.11 Myr, Ė sp = erg s 1 GBT: radio pulsar same position and period GeV pulsar, and a Be star Extreme Astrophysics Introduction 7
8 Field around PSR J Suzaku VLA 6 cm [Murakami et al. 2011, PASJ, 63, 873] [Butt et al. 2008, MNRAS 385, 1764] Extreme Astrophysics Introduction 8
9 Observations VLA June 28, 2010 Two frequency bands centered at 4.4 and 7.8 GHz D configuration EVN Observations on 2010, 2011, and GHz Pulsar gating Chandra Archival data, kev band, 48.7 ks observation on 2004 July 12 with the Advanced CCD Imaging Spectrometer (ACIS) detector. Extreme Astrophysics Observations 9
10 Observations VLA June 28, 2010 Two frequency bands centered at 4.4 and 7.8 GHz D configuration EVN Observations on 2010, 2011, and GHz Pulsar gating Chandra Archival data, kev band, 48.7 ks observation on 2004 July 12 with the Advanced CCD Imaging Spectrometer (ACIS) detector. Extreme Astrophysics Observations 9
11 Observations VLA June 28, 2010 Two frequency bands centered at 4.4 and 7.8 GHz D configuration EVN Observations on 2010, 2011, and GHz Pulsar gating Chandra Archival data, kev band, 48.7 ks observation on 2004 July 12 with the Advanced CCD Imaging Spectrometer (ACIS) detector. Extreme Astrophysics Observations 9
12 VLA VLA: Extended radio emission Extreme Astrophysics VLA 9
13 Extended radio emission: a PWN δj PSR J VLA 4.4 GHz s 16 s 14 s α J s 20 h 32 m 10 s Extreme Astrophysics VLA 10
14 Extended radio emission: a PWN δj PSR J VLA 4.4 GHz VLA 7.9 GHz s 16 s 14 s α J s 20 h 32 m 10 s Extreme Astrophysics VLA 10
15 Radio spectrum 4.0 Flux density [mjy] 1.0 GMRT GBT VLA GBT Frequency [GHz] Pulsar spectrum: S ν = (0.36 ± 0.02)(ν/GHz) 1.6±0.1 mjy Insignificant contribution from the pulsar: α = 0.4 ± 0.4 Extreme Astrophysics VLA 11
16 EVN EVN: Pulsar proper motion Extreme Astrophysics EVN 11
17 PSR J proper motion δj s 16 s 14 s α J s 20 h 32 m 10 s µ α cos δ = 2.0±2.0 mas yr 1 µ δ = 10.8 ± 2.0 mas yr 1 α J = 20 h 32 m ±.002 s δ J = ± 0.02 Extreme Astrophysics EVN 12
18 PSR J proper motion δj s 16 s 14 s α J s 20 h 32 m 10 s µ α cos δ = 2.0±2.0 mas yr 1 µ δ = 10.8 ± 2.0 mas yr 1 α J = 20 h 32 m ±.002 s δ J = ± 0.02 Extreme Astrophysics EVN 12
19 PSR J proper motion δj s 16 s 14 s α J s 20 h 32 m 10 s µ α cos δ = 2.0±2.0 mas yr 1 µ δ = 10.8 ± 2.0 mas yr 1 2D velocity: km s 1 at kpc Extreme Astrophysics EVN 12
20 Galactic velocity vrad [km s 1 ] vz [km s 1 ] vcir [km s 1 ] Components of the Galactic and peculiar velocity of PSR J The grey areas indicate the expected Galactic velocity for young stars. (II) Assuming radial velocity of: +100 km/s (dashed line) -100 km/s (dotted line) 120 vpec [km s 1 ] Distance [kpc] The velocities are not compatible with the expected ones from Galactic rotation Extreme Astrophysics EVN 13
21 Galactic velocity vrad [km s 1 ] vz [km s 1 ] vcir [km s 1 ] Components of the Galactic and peculiar velocity of PSR J The grey areas indicate the expected Galactic velocity for young stars. (II) Assuming radial velocity of: +100 km/s (dahsed line) -100 km/s (dotted line) 120 vpec [km s 1 ] Distance [kpc] The velocities are not compatible with the expected ones from Galactic rotation Extreme Astrophysics EVN 14
22 Widefield 36 δj Contours: JVLA 4.4 GHz Black Cross: EVN, pulsar Black dots every 5000 yr s 20 s 32 m 00 s α J h 31 m 40 s Extreme Astrophysics EVN 15
23 Widefield δj s VERITAS MAGIC HEGRA 20 s 32 m 00 s 20 h 31 m 40 s α J2000 Contours: JVLA 4.4 GHz Black Cross: EVN, pulsar Black dots every 5000 yr Red ellipse: Fermi The past trajectory of PSR J coincides with the measurement of the CoG of the TeV emission measured with MAGIC, which is compatible with the measured positions from HEGRA and VERITAS Extreme Astrophysics EVN 16
24 Chandra Chandra: diffuse X-ray emission Extreme Astrophysics X-ray 16
25 Diffuse X-ray emission 29 δj Contours: JVLA 4.4 GHz Cross: EVN, pulsar Red Crosses: Chandra s 16 s 12 s α J h 32 m 08 s Extreme Astrophysics X-ray 17
26 Diffuse X-ray emission 29 δj Contours: JVLA 4.4 GHz Cross: EVN, pulsar Red Crosses: Chandra Color scale: diffuse Chandra s 16 s 12 s α J h 32 m 08 s Extreme Astrophysics X-ray 18
27 X-ray/gamma-ray correlation Correlations of the X-ray and gamma-ray fluxes with Ė and τ c: Ė sp = erg s 1 L X = erg s 1 or F X = erg cm 2 s 1 τ c = 0.11 Myr F γ /F X 1000 L γ = erg s 1 [Mattana et al ApJ ] Extreme Astrophysics Correlation 19
28 X-ray/gamma-ray correlation Correlations of the X-ray and gamma-ray fluxes with Ė and τ c: Ė sp = erg s 1 L X = erg s 1 or F X = erg cm 2 s 1 τ c = 0.11 Myr F γ /F X 1000 L γ = erg s 1 [Mattana et al ApJ ] Extreme Astrophysics Correlation 19
29 Diffuse X-ray emission 29 δj The diffuse emission could be: Partially from the PWN itself. Unrelated source. Field young stars? e escaping from the shock? s 16 s 12 s α J h 32 m 08 s Extreme Astrophysics Correlation 20
30 Scenario High speed pulsar forms a shock at 1. High energy particles are accelerated and escape the shock region. If leptonic, they could be the responsible of the TeV source through IC in the Thomson regime off CMB and IR galactic photons with energy density u CMB IR 1 ev. Diffusion coefficient of D cm 2 s 1, t diff kyr. Particles are advected by the shocked flow in the opposite direction to the pulsar motion. These relativistic particles produce radio (detected) and X-ray emission (not detected yet). The size of the TeV source is compatible with a projected velocity of 100 km s 1. Extreme Astrophysics Scenario 21
31 Conclusions The radio morphology strongly resembles that of a PWN. The positional coincidence between the pulsar and the origin of this elongated radio structure suggests a physical association. This is supported by the proper motion of the pulsar, opposite to the radio structure. The pulsar space velocity is not compatible with the Galactic rotation. Probably formed with a kick. The absence of diffuse X-ray emission overlapping the elongated radio structure could be explained by the low flux expected. The extended X-ray emission detected with Chandra and Suzaku remains unclear. (Associated with the Be stars in the field?). Extreme Astrophysics Conclusions 22
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