超新星遗迹和相关联天体的21 厘米中性氢观测

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							超新星遗迹的射电巡天观测和
 甚高能伽玛射线源研究

     田文武


    2008年6月5日在北京大学的报告
       射电天文的重大发现
• 1951年,星际HI谱线
• 1965年,3K微波背景
• 1967年,脉冲星, VLBI
• 1968年,星际分子
• 1971年,视超光速运动
• 1974年,脉冲双星/引力波


• ….
                      概要
• 21厘米中性氢原子(HI)谱线银道面巡天简介及建立新方法
  (Tian & Leahy方法)获得可信赖的超新星遗迹和相关联天体
  的距离(或范围)
• 超新星遗迹和分子云的相互作用导致很多天体物理现象,如
  加速带电粒子到相对论能量, 产生可以观测到的TeV伽玛射
  线. 测定天体的距离可以直接检验超新星遗迹是河内宇宙线
  粒子起源处的合理性
• 实例: 四个超新星遗迹和TeV源相关联系统:G29.7-0.3/PSR
  J1846-0258/HESS J1846-029, G21.5-0.9 /PSR J1833-
  1034/HESS J1833-105, G23.3-0.3/HESS 1834-087,G353.6-
  0.7/HESS J1731-347; 一个含异常X-光线脉冲的年青超新星
  遗迹 G27.4+0.0 /AXP 1E1841+045;一个正与临近大CO分子
  云相互作用的超新星遗迹 G18.8+0.3; 及一个产生1720兆赫
  兹OH脉泽辐射的年青超新星遗迹 G21.8-0.6.
21-cm HI observations in the Milky Way disk
  1420MHz and 13CO data ( + X-ray data)
1420 MHz data from the VLA • 13CO(J=1-0) data from the
Galactic Plane Survey (Still et Galactic ring survey (Jackson et
al. 2006, AJ, 132, 1158):
                                 al.2006, ApJS, 163, 145) by the
Range:18<l<67d, -1.3<b<2.3d      Five College Radio Astronomy
FWHM: 1'×1'×1.56 km/s            Observatory 14m telescope:
Velocity range:-113– 165 km/s    Range:18<l<56d, -1<b<1d
rms :2 K per channel
                                 FWHM:46"x46"x0.21 km/s
Short-spacing information for
                                 rms:~ 0.13 K per channel.
the H I line emission from
observations with the 100m       Velocity range: -5-- 135 km/s
Green Bank Telescope
                                 (<=40d), -5-- 85km/s(>=-40d)
 An example to build absorption spectra to Kes 75 (a TeV source)



                                       21 cm HI map from VLA+GBT
                                       observations with contours (28 40
                                       60 100 k) overlaid




  1420 MHz map from VLA
  D-array observations.


Ton (v)-Toff(v)=(Ts-Tbg)(1-e^{-tau})
solid-line box ---> Ton(v)
Annulus background Toff(v)
• HI+CO13 spectra show that the highest absorption velocity~95 km/s, absence of
  absorption at ~102 km/s, the tangent point velocity ~110 km/s. So d ~ 5.1 to 7.5 kpc
• Rotation

 curve of

 Milky Way

 stays flat

 with

 distance
Calculated radial velocity as a function of distance along a
line of sight in the Galactic plane at l = 29.7 degree
Formula: Vr= Ro sin l (V(R)/R – Vo/Ro). V(R):circular orbit
speed of a star; R:Galactocentric radius; Vr:radial velocity
The long-standing puzzle on Kes 75/PSR J1846-0258 is resolved
 (Leahy & Tian, 2008, A&A, 480, L25. 已7次独立引用, 改写了前面的结
        果:Becker & Helfand, 1984, ApJ, 283, 154,被引用36次)

1. Significant distance revision from ~19 kpc to ~ 6 kpc for Kes 75
gives a normal explosion energy (~2x10E51 erg) from a core
collapse, contrary to the highly implausible value (~10E53 erg) for
an extremely high X-ray luminosity for Kes 75 (~4x10E37 ergs /s)
obtained previously due to d ~ 19 kpc.
2. Small radius ~ 3 pc (1.6') for Kes 75 argues that it harbors a
Crab-like rotation powered young pulsar J1846-0258 and PWN
(723--884 yr) , rather than the previous inferred, much higher ratio
of the pulsar-plus-nebula luminosity to spin-down luminosity.
Kes 73 new results:
1.Absorption features
appear up to tangent
point velocity (~110
km/s)
2.At 114 km/s, the HI
distribution is quite
inhomogeneous.
3.The HI feature at 84
km/s is at the far
distance

Conclusion: Kes 73 is
in front of the HI at
84 km/s, but beyond
the tangent point.
                                       ~84 km/s ~110 km/s tangent point
• HI+CO spectra confirm the
  above conclusion.
• The CO cloud (~89 km/s) is
  behind Kes 73. Limits to
  distance of Kes 73/AXP
  1E1841-045 between the far
  distance (9.4 kpc) of 89 km/s
  and the tangent point (7.5 kpc)
  which was used as an upper
  limit in past 20 yrs.
• Kes 73 has a refined age of 500
  to 1000yr, the AXP has a larger
  50% X-ray luminosity.
• Tian & Leahy, ApJ, 2008, 677,
  692
                                    ~89 km/s
     •           SNR/Cloud interaction
                                         • 1. Detection of high energy gamma
                                           ray and non-thermal X-ray emission
                                         • 2. Detection of 1720 MHz shock-
                                           excited OH masers ---"signposts" of
                                           SNR-molecular cloud interactions.
                                         • 3. Detection of high line rates CO(2-
                                           1)/CO(1-0) and broad wings of 10–
                                           20 km/s in CO and other molecular
                   Emit TeV gamma-rays
                                           spectra (Moriguch et al. 2005, ApJ,
                                           631, 947).
                                         • 4. Detection of shocked H2 emission
                                           from the system at near-infrared band
                                           (Reach et al. 2005, ApJ, 618, 297).
 Schematic of an expanding SNR • Direct method: Determine distance
interacting with an adjacent     to a SNR/CO Cloud system by
                                 HI+CO obs.
   molecular cloud (Wardle &
   Yusef-Zadeh 2002)
  The distance to Kes 69 and G21.5-0.9
Green A.J. et al. (1997, AJ, 114, 2058) suggested a far distance (11.2
kpc) of the 1720 MHz OH maser velocity 69.3 km/s by HI+OH obs.

                           Old OH
                           maser at
                           69.3km/s
                           New OH
                           Maser at                      1       pwn

                           ~84km/s
                                                     G21.5-0.9
 X-ray (contour --ROSAT PSPC)+radio
 (grey from NVSS) image from Yusef-
 Zadeh et al. (2003, ApJ, 585, 319)          New VLA 1420 MHz map
        Kes 69
• HI spectrum: max velocity of
  absorption ~86 km/s; HI emission
  feature at 113 km/s with no
  respective absorption.
• CO image + spectrum: adjoining
  cloud at ~ 85 km/s, no prominent
  cloud around 70 km/s towards the
  bright southern shell.
• New detected 1720 MHz OH maser
  at velocity 80-86km/s from within
  the southern shell of Kes 69.
• Conclusions: distance of ~5.5 kpc
  to Kes 69, and physical interaction
  between Kes 69 and adjoining
  cloud.
                          (from Jack Hewitt)
                                         Spitzer image




        VLA D-Array            y         GBT map




Integrated1720 MHz line intensity   OH maser Vo=84 km/s
G21.5-0.9 and PMN J1832-1035




              1. The highest absorption velocity~66
              km/s, no absorption at~71 and 86 km/s
              2. G21.5-0.9 is likely at 4.4 – 4.8 kpc
              (near side of ~ 71 km/s) or possibly at
              4.4 – 8 kpc (far side of ~86 km/s)
http://www.mppmu.mpg.de/~rwagner.sources
                            The thick-solid line shows the total non-
 vFv spectrum of a young
                               thermal flux.
SNR with an age 10^3 yrs
                            Hadronic emissions are Pion-decay gamma-
                            rays (thin-solid), synchrotron (dot-dashed)
                            and bremsstrahlung emission (short-and-
                            long dashed) from secondary electrons
                            produced by charged pion.
                            Leptonic emissions are synchrotron (long-
                            dashed), inverse-Compton (dotted) and
                            bremsstrahlung (short-dashed) emission
                            by primary electrons.
    an old SNR case        an old SNR-a GMC         an illuminated GMC
The HESS J1731-347 image ( Aharonian et al. 2008, A&A, 477,
353); Contours start at 4 sigma in 1 sigma steps, which is of
gamma-ray excess counts smoothed with a Gaussian filter with
standard deviation 0.1 degree. Energy range:0.50 to 80 TeV.
                                 A power-law fit to the spectral data
                                 (E=N0E^{-Г}),Г=2.26±0.10
     Two SNR and TeV HESS source Systems
1. Discovery of the Radio and X-ray counterpart of TeV
   gamma-ray Source HESS J1731-347
    W.W. Tian(1,2), D.A. Leahy(2), M. Haverkorn(3), B. Jiang(4)
    (2008 June 1, ApJL, 679, 85)
•   1. National Astronomical Observatories of China, CAS, China
•   2. Department of Physics & Astronomy, Uni. of Calgary, Canada
•   3. Astronomy Department, Uni. of California-Berkeley, USA
•   4. Department of Astronomy, Uni. of Massachusetts, USA

2.First evidence: an old SNR encounters a GMC to emit
    TeV gamma-rays in the cloud: W41/HESS J1834-087
    W.W. Tian(1,2), Z, Li(4), D. Leahy(2), Q.D. Wang(4)
    (2007, ApJL, 657, 25. 已13次引用, 其中9次独立引用):
                       SNR G363.6-0.7?
•   Left: the continuum image of G353.6-0.7 at 1420 MHz from the Southern
    Galactic Plane Survey (SGPS, ATCA data) with a beamsize of 100 arcsec and a
    sensitivity of < 1 mJy/beam (Haverkorn et al. 2006, ApJS, 167, 230)
    Right: the 843 MHz image from the Molonglo GPS with a beamsize of 43
    arcsec and a sensitivity of 1~ 2 mJy/beam (Green et al. 1999, ApJS, 122, 207)
        X-ray and IR Images: a likely SNR
Left: ROSAT PSPC image (0.1-2.4 kev), centred at l=353.55, b=-0.6
integration time of 300 s, Signal-to-Noise ratio ~ 5
Right: 8 micro mid-infrared image, centred at l=353.5, b=-0.65 from the
GLIMPSE Legacy survey with resolution of ~2 arcsec (Benjamin et al.
2003, PASP, 115, 953). No thermal emission down to a limit of 0.4 mJy
(5 sigma), G353.6-0.7 is not an HII region!
              Spectral Index of G353.6-0.7
Total flux density estimayes of 2.2±0.9 Jy at 1420 MHz and 1.4±0.3 Jy at 5
GHz (Parkes observations, Haynes et al. 1978, Austr. J. of Phys. Suppl. 45, 1)
by same method, give = 0.4(- 0.6/+0.5), favour a non-thermal feature.
The 843 MHz data misses too many low spatial frequency components to be
used to obtain a reliable flux density.
ACTA+Parkes image. The ring shows        Azimuthally averaged flux over the low
the boundary of SNR G353.6-0.7.          half of G353.6-0.7 as a function of
                                         radius from the center of the remnant.
            Distance to G353.6-0.7
Too faint to obtain HI absorption spectrum of the new SNR. HII
region G353.42-0.37 is adjacent to the SNR. The HI absorption
spectrum features in the range of 9 to -24 km/s show G353.42-
0.37 is at the distance (~ 3.2 kpc) of its recombination line
velocity (~ -16 km/s).            A number of HESS sources are detected
                                   where high-energy particle accelerators
                                   are located near H II regions, and other
                                   such accelerators without proximate
                                   sources of low-energy photons are weak
                                   or undetected at TeV energies, Helfand et
                                   al. (2007) suggested that TeV emissions
                                   of HESS sources could originate from
                                   inverse Compton scattering of the
                                   starlight from the nearby H II regions.
                                   SNR G353.6-0.7 may be at ~3.2 kpc.
Overlapping Radio (grey)+X-ray (red)+gamma-ray
          (green) images of G353.6-0.7
                              1. The radio and X-ray
                              morphologies of G353.6-0.7
                              near-perfectly march the
                              outline of HESS J1731-347.
                              2. The low half seen in X-
                              rays and upper half not seen
                              in X-rays is likely due to
                              clouds' absorption, which is
                              revealed by the 12CO
                              column density increasing
                              towards the Galactic plane.
              How old is G353.6-0.7?
1. An old SNR: a large angular size of 0.5 degree and a
physical size of ~28 pc in diameter (assuming a distance of
~ 3.2 kpc); faint radio and X-rays.

2. Ambient density n0 ~5 cm-3, estimated by known flux
(~1.2E-11 cm-2 s-1, assuming a conversion efficiency ~ 0.1
and explosion energy 10E51 ergs, Aharronian et al. 2006
ApJ, 636, 777),

3. An age of ~27,000 yr, based on a Sedov model (Cox
1972, ApJ,178, 159), it is entering a radiation phase.

4. It is not too old < 100000 yrs, because the X-rays are
visible in G353.6-0.7 and an old SNR is expected to emit few
               W41/HESS J1834-087
• XMM-Newton observations show diffuse X-ray emission
  within the HESS source J1834-087--- this suggests an
  association between the X-ray and TeV gamma-ray emissions.
• High-resolution 13CO images reveal a giant molecular cloud
  (~ 78 km/s) at the center of W41--likely associated with W41.
• Probably, the first evidence that an old SNR encounters a
  GMC to produce TeV gamma-rays
• New results (Leahy &Tian 2008, AJ): determining distances
  to the W41/cloud system support that such interaction is
  physical by analyzing HI and 13CO spectra.
Radio Images of W41/molecular cloud:
1420 MHz continuum map             13CO map from Galactic Ring Survey:
36'x30' in size, F1420=60+/-8 Jy   a GMC at the center of W41: MH2~10^5 M0
Alpha>=0.43 (330 -1420 MHz)
                                   NH2 ~10^22 (cm^-2), no ~ 10^3 (cm^-3)
(Fv ~ v^(-alpha)
             XMM-NEWTON Observations of W41
An EPIC-pn intensity image in 0.3-1.5       The central part of W41 in 1.5-7
keV. 15 point-like sources are detected     keV. A region of enhanced intensity
also. Red circle represents HESS            is clearly present coincident with the
J1834-087; small green circle illustrates   HESS source, apparently diffuse.
the region for x-ray spectrum.              Contours of 13CO emissions at 1.2,
                                            1.4, 1.8 and 2.1k.
     W41/CO cloud physical interaction

                               Two nearby CO features:
                               at ~77 km/s and ~95 km/s




• The maximum velocity of
  HI absorption:~78 km/s. No
  absorption at ~95 km/s.
  一个正与临近大CO分子云相互作用的超新星遗迹
           G18.8+0.3
          Tian, Leahy & Wang, 2007, A&A, 474, 541
• Previous observations         • HI+13CO observations:
  (12CO + HI + OH, Dubner         constrain distance to Kes 67;
                                  a GMC at 20km/s is
  et al. 1996, AJ, 111, 1304;     physically adjoining with the
  2004 A&A, 426, 201):            SNR.
• 1. Morphological agreement    • ROSAT PSPC: a diffuse X-
  between one 12CO clump          ray feature apparently
  and the SNR shock front.        associated with part of the
                                  radio shell of the SNR.
• 2. Detection of high line
  rates 12CO(2-1)/12CO(1-0)     • New 13CO observation: clear
                                  morphological agreement
  in a clump.                     between the SNR and an
• A conclusion: a possible        adjoining cloud; broadened
  interaction between SN          profile seen in the 13CO
  shock and an adjoining          emission spectrum.
  molecular cloud               • There likely exists a
                                  physical interaction!
  Radio and X-ray images of Kes 67
 1420 MHz image            HI Image at 18.3 km/s




CO image at 19.8 km/s   ROSAT PSPC image (0.5-2.4 kev)
                    HI and 13CO spectra
1.The largest velocity absorption feature at the tangent point gives a lower
distance limit of 7.6 kpc.
2. Absence of absorption at negative velocities gives upper limit of 15.2 kpc.
3. The broadened profile at ~20 km/s in the 13CO spectrum indicates a
 likely SNR/CO cloud interaction and gives a distance of ~12 kpc.
                     Tangent point

                                                          ~20 km/s
                     Summary
• Using HI+13CO spectra determine distances to seven
  SNR/PSR/HESS systems: Kes 75~ 6 kpc; Kes 69 ~5.5
  kpc, Kes 7--7.5-9.4 kpc, W41--3.9-4.5 kpc, Kes 67~12
  kpc, G21.5-0.9--4.4-4.8 kpc, G353.6-0.7~3.2 kpc
• Some values differ greatly from previously published
  values, partly because our methods resolve the near/far
  distance ambiguity, partly due to better discrimination
  against HI emission differences in background spectra.
• Determining distances to SNR/Cloud/TeV HESS
  source systems help to trace Galactic CRs origin.

						
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