Pulsar Rotation Measures and Galactic Magnetic fields Grateful
- Slides: 69
Pulsar Rotation Measures and Galactic Magnetic fields Grateful to cooperators Jin. Lin Han National Astronomical Observatories Chinese Academy of Sciences Beijing 100012, China hjl@bao. ac. cn P. Demorest R. N. Manchester W. van Straten A. G. Lyne G. J. Qiao K. Ferrier
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
Pulsar Distribution in the sky
Galactic Distribution of Pulsars: How do you get Distances?
Interstellar medium: Clouds & large-scale structure?
Interstellar medium: Clouds and turbulent structure ?
Ionized Interstellar Medium+ moving pulsars Warm ionized medium (WIM): n ~ 0. 1 cm-3; T ~ 8000 K; f ~ 0. 2 WHAM�
Effects of Interstellar Medium • • DM EM RM SM ds ne 2 ds ne. B|| ds Cn 2 Dispersion Measure Emission Measure Rotation Measure Scattering Measure Spectrum = Cn 2 q- , q = wavenumber (temporal spectrum not well constrained, relevant velocities ~ 10 km/s) = 11/3 (Kolmogorov value) Scales ~ 1000 km to > pc
Dispersion Measures L b H Uniform slab of density Ne If L > H cos(b) DM = Ne H cos(b) Ne H = 20 pc cm-3 If L < H cos(b) DM = Ne. L < Ne H cos(b) DM DM = 20 cosec b Galactic Latitude
Dispersion & Independent Pulsar Distances Independent Dist + DM | i=1, N Ne 2001 model + DM Dist? Indep. Dist. Obs Number Parallaxes: Interferometry timing optical Associations HI absorption DM + ne model ~13 ~5 ~1 Comments 1 mas @ 1 kpc 1. 6 s @ 1 kpc HST, point spread function SNRs 8 false associations GCs 16 LMC, SMC ~8 bright pulsars, 74 galactic rotation model all radio pulsars (~ 1400) ISM perturbations
NE 2001 • Goal is to model ne(x) and Cn 2(x) Fne 2(x) in the Galaxy • Input data = {DM, EM, SM, [DL, DU] = distance ranges} • Prior input: – Galactic structure, HII regions, spiral-arm loci – Multi- constraints on local ISM (H , Na. I, X-ray) • Figures of merit: – N> = number of objects with DM > DM (model) (minimize) – Nhits = number of LOS where predicted = measured distance: d(model) [DL, DU] (maximize) – L = likelihood function using distances & scattering (maximize) • Basic procedure: get distances right first, then get scattering (turbulence) parameters From J. Cordes
NE 2001 • x 2 more lines of sight (D, DM, SM) [114 with D/DM, 471 with SM/D or DM] (excludes Parkes MB obj. ) • Local ISM component (new) (new VLBI parallaxes) [12 parameters] • Thin & thick disk components (as in TC 93) [8 parameters] • Spiral arms (revised from TC 93) [21 parameters] • Galactic center component (new) [3 parameters] (+auxiliary VLA/VLBA data ; Lazio & Cordes 1998) • Individual clumps/voids of enhanced d. DM/d. SM (new) [3 parameters x 20 LOS] • Improved fitting method (iterative likelihood analysis) penalty if distance or SM is not predicted to within the errors From J. Cordes
Model Components e v a h e ! t i e t a d p u to W Ne 2001 model + DM Dist?
Pulsars as best probes for Galactic B-field • Polarized + no intrinsic RM: Faraday rotation: • ne: can be measured: » <== the delay tells DM » » » the rotation of position angles tells RM value ==> » �����Average field strength » can be directly derived RM>0, field toward us
Pulsars: Best probes for Galactic magnetic field Widely spread in the Galaxy ! Parkes PSR survey 3 -D B-field structure!
Why to study the B-field of our Galaxy • Galaxy: a necessary key step from Sun to Universe! • Important hints for B-origin: primordial or dynamo? • Important roles in star formation • Hydrostatic balance & stability in ISM: B 2/8π= ρ v 2/2 B~106 G, ρ=1024 gcm-3, v=10 km s-1 (eg. Boilers & Cox 1990 for details) • Key info for cosmic rays – propagation! • Foreground for CMB? ! Thanks to WMAP To understand the Galactic B-field, we have to measure first ! Knowledge on the Galactic B-field is far from complete!
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
Paired probes to measure B-field in a region RM ∝ ∫ n*e B// ds DM ∝ ∫ n* e ds Sun d 2 If many pairs, do average, or Fit together! d 1 d 2 Analysis is not limited to modeling B all the path, path but can measure B in the region between! Significant improvement! No worry about foreground bubbles! Less sensitive on Dist!
Major observations of pulsar RMs Authors Hamilton & Lyne (1987) Rand & Lyne (2004): Qiao et al. (1995) Han et al. (1999) Weisberg et al. (2003) Han et al. (2006): Noutsos et al. (2008) g i b t No. of RMs No. New RMs 163 119 27 27 48 33 63 54 36 17 223 196 150 43 477 400 ! ep st 1 s ! p e s t s r g u bi ho es d 0 rk n 2 50 Pa > t a Han et al. (2010 to submit!):
Pulsar RMs observed by others |b| < 8 degree
63+223 RMs by Parkes (Han et al. 1999, 2006) |b| < 8 degree
63+223+477 RMs by Parkes +GBT (Han et al. 1999, 2006, 2009) |b| < 8 degree
Pulsar RMs observed by others |b| > 8 degree
63+223 RMs by Parkes (Han et al. 1999, 2006) |b| > 8 degree
63+223+477 RMs by Parkes +GBT (Han et al. 1999, 2006, 2009) |b| > 8 degree
Paired probes to measure B-field in a region RM ∝ ∫ ne B// ds DM ∝ ∫ ne ds d 2 If many pairs, do average, or Fit together! d 1 d 2 Analysis is not limited to modeling B all the path, path but can measure B in the region between! Significant improvement! No worry about foreground bubbles! Less sensitive on Dist!
Measuring the B-field in the Norma arm red: new measurements by Parkes 64 m telescope Han et al. 2002, Ap. J 570, L 17
Measuring B-field in tangential regions! Random B causing the scattering of data, � gives uncertainties of <B> (Han et al. 2006, Ap. J 642, 868)
Measured magnetic field in the Galactic disk by pulsar RM/DM (Han et al. 2006, Ap. J 642, 868) • always counterclockwise in arm region! • clockwise in interarm region ? • More data still needed!
Measured Radial dependence of regular field strength (Han et al. 2006, Ap. J 642, 868) Uncertainties reflect random fields!
RMs from radio sources behind the Galactic plane: Consistent with B-Structure from pulsar data! Haverkorn et al. 2006 Brown et al. 2007 Han et al. 2006 • PSR and EGRs data show a consistent B-structure! • Dominant RM contribution from tangential regions!
Han et al. 2010, Ap. J to be submitted。 1024 Pulsar RMs s u e rc io d ra so ! f k o s s di M R nd i h Be
(Han et al. 2010, Ap. J to be submitted。 1024 Pulsar RMs )
(Han et al. 2010, Ap. J to be submitted )
Measured B-structure in the Galactic disk (Han et al. 2010, Ap. J to be submitted )
RMs of background radio sources for B-field in the GC region (Roy et al. 2008) Sun
Measured B-structure in the Galactic disk √ √ ? X (Han et al. 2010, Ap. J to be submitted )
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
Measuring the B-field fluctuationvs scales
Many Simulations of dynamos ----check spatial B-energy spectrum & its evolution e. g. Magnetic energy distribution on different spatial scales (k=1/λ) Many papers by • • N. E. L. Haugen, A. Brandenburg, W. Dobler, …. . A. Schekochihin, S. C. Cowley, S. Taylor, J. Moron, …. . E. Blackman, J. Maron …. . Others …. . No measurements of the B-energy spectrum !
Spatial magnetic energy spectrum of our Galaxy (Han et al. 2004, Ap. J 610, 820) Email from A. Minter By pulsar RM/DM Flatter B-energy spectrum at scales larger than the ISM energy-injection-scale! Minter & Spangler 1996 λ< ~4 pc: 3 D Kolmogorov 80>λ> ~4 pc: 2 D turbulence?
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
RM Sky: Anti-symmetry! Outliers significantly different from surroundings been filtered RM<0 : <B> away from us + -- -- + RM>0 : <B> to us Milky Way: The largest edge-on Galaxy in the sky Pulsars and extragalactic radio sources as probes
Anti-symmetric RM sky: A 0 dynamo? (Han et al. 1997, A&A 322, 98) Evidence for global scale • High anti-symmetry to the Galactic coordinates • Only in inner Galaxy • nearby pulsars show it at higher latitudes Implications • Consistent with field configuration of A 0 dynamo • The first dynamo mode identified on galactic scales Sun
RM sky: Antisymmetry is confirmed! Notice: RM estimated from only 2 IFs of NVSS data Individually: cannot trust! Collectively: Ok! + -- -- +? Taylor et al. (2009)
RMs of Extragalactic radio sources RMobs = RMintrinsic + RMInter. Galactic + RMMilky. Way Common term! • RMintrinsic : RM intrinsic to the source; – They never know each other: uncorrelated Random! – Location of emission regions: Beam size? • RMInter. Galactic : RM from intergalactic space; – weak correlated if with same intervening medium – Small values ? ? • RMMilky. Way : Foreground RM from our Galaxy; – Correlated ~10 o with same intervening ISM – Strongly depends on the Galactic coordiantes!
Local vertical components: frompoloidal field? North Galactic Pole ����������������Unique measurement Preferably of Vertical B-component positive � Mao et al. 2010 Ap. J South Galactic Pole Preferably negative Bv= 0. 2~ 0. 3 G� pointing from SGP to NGP (Effect of the NPS discounted already!)� (see Han & Qiao 1994; Han et al. 1999)
Measured B-strength in halo by 285 pulsars (Han et al. 2009, Ap. J to be submitted )
Measured B-strength in halo by 285 pulsars (Han et al. 2009, Ap. J to be submitted )
Measured B-strength in halo by 285 pulsars B~ G u 1 -2
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
Connection of Galactic B-fields of large and small scales Beck et al. 1991, IAUS 146, 209
Connection of Galactic B-fields of large and small scales Li et al. 2006: Ap. J 648, 340 (Results of SPARO 2003) 2003 • Mapped large-scale magnetic fields in four GMCs Galactic plane • Statistically significant correlation with the orientation of the Galactic plane. • Field direction tends to be preserved during the process of GMC formation.
B-field from maser spots Han & Zhang (2007 , A&A 464, 609 ) • Collect Zeeman splitting data of maser spots in HII and star formation regions • Spots in one region always have the same field orientation!
The Galactic distribution of Zeeman data Structure in distribution of field directions In situ au-scale-B correlated with kpc-B! Reversals: preserved from ISM to maser core! Blue: Counterclockwise field Red: Clockwise field Han & Zhang 2007 A&A 464, 609 We need more data, and better determined distances!
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
Pulsar birth & SN explosion (Hobbs et al. 2005) Guitar Nebula Asymmetric explosion gives kick velocity! PSR B 2224+65 Measured <V 2 D> = 211 km s-1 <V 3 D> = 4<V 2 D>/ = 2<V 1 D> (Cordes et al. 2003)
Ionized Interstellar Medium+ moving pulsars Warm ionized medium (WIM): n ~ 0. 1 cm-3; T ~ 8000 K; f ~ 0. 2 WHAM�
Strong Interstellar Scintillation (ISS) • Below ~ 3 GHz. Interstellar Scintillation is strong, having an rms change in flux density > mean flux density • Two Time scales: – Diffractive ISS td ~ so / V rms flux ~ mean flux – Refractive ISS tr ~ L qscatt / V rms flux < mean flux For typical pulsar distance: td ~ 5 -50 min (f+1. 2) dnd ~ DMx (f. GHz)4. 4 tr ~ 5 -100 days (f-2. 2 ) dnr ~ fo For an extended scattering medium x ~ 2. 2 but in observations of pulsars x ~ 2 - 4
Scattering Disc and Refractive ISS Sr=Lqd L qd When the screen has a wide range of scales, the largest scale that can cause a fluctuation in amplitude is Lqd = sr This is called refractive scintillation
Angular broadening of a point radio source 330 MHz 610 MHz
Scattering and pulse-broadening
Scattering and pulse-broadening 0. 43 Bhat et al. 2004 1. 18 1. 48 2. 4 GHz Mitra & Ramachandran (2001):
Scattering and Polarization ? ? ? B 1838 -04 Li & Han 2002
Scattering and Polarization ? ? ? B 1841 -05 Li & Han 2002
Outlines • Pulsars as probes for interstellar medium • Why to study magnetic fields • Pulsar RMs for Disk fields: Large-scale reversals – Field structure – Field strength – Field fluctuation • RM sky: Antisymmetryfor Galactic halo fields – Confirmed – Measured by pulsar RM/DM ! e n o D • Small-scale and large-scale fields: connections – Zeeman B of masers ~? ~ Large-scale B-field in disk • Scattering for polarized signal? Yes.
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