Presentation is loading. Please wait.

Presentation is loading. Please wait.

Magnetic fields in our Galaxy JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China Thanks for cooperation.

Similar presentations


Presentation on theme: "Magnetic fields in our Galaxy JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China Thanks for cooperation."— Presentation transcript:

1

2 Magnetic fields in our Galaxy JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China hjl@bao.ac.cn Thanks for cooperation with Dick Manchester Dick Manchester (ATNF, Australia), G.J. Qiao G.J. Qiao (PKU, China), A.G. Lyne A.G. Lyne (Jodrell Bank, UK), (K. Ferriere: (K. Ferriere: Obs. Midi-Pyr. France)

3 Magnetic fields in our Galaxy What RMs of pulsars & EGRes can tell us? Some background, remindingSome background, reminding Knowledge 10 years agoKnowledge 10 years ago Current knowledgeCurrent knowledge –Central field & halo field –disk field »directions »strength –spatial magnetic energy spectrum We advanced a lot of knowledge on magnetic fields of our Galaxy in last 10 years! --- More coming.

4 Observational tracers of magnetic fields perpendicular field in 2 or 3 kpc Polarization of starlight: perpendicular field in 2 or 3 kpc orientation // B ⊥ ------------- 9000 stars parallel field, in situ (masers, clouds) Zeeman splitting : parallel field, in situ (masers, clouds) △ ∝ B // ------ 30 masers perpendicular field Polarization at infrared, mm: perpendicular field orientation // B ⊥ ------------- star formation regions vertical field structures (added) Synchrotron radiation: vertical field structures (added) total intensity S ∝ B ⊥ 2/7, p% ∝ B ⊥ u 2 / B ⊥ t 2 parallel field, integrated (the halo & disk) Faraday rotation: parallel field, integrated (the halo & disk) RM ∝ ∫ n e B // ds ------ 550 pulsars + >2000 EGSes

5 9000 stars have polarization measured mostly nearby (1~2kpc) polarization percentage increases with distance Zweibel & Heiles 1997, Nature 385,131 Berdyugin & Teerikorpi 2001, A&A 368,635 Starlight polarization: local field // arm

6 Zeeman Effect: B in molecular clouds Bourke et al. 2001, ApJ 554, 916 >30 people working for >30 years, get <30 good measurements! Difficult & Bad Luck! Difficult & Bad Luck!

7 Nothing to do with large-scale B-field?! Maser B-fields: Nothing to do with large-scale B-field?! n e : ISM: 1cm -3 ==> GMC: 10 3 cm -3 ==> OH-maser: 10 7 cm -3 Fish et al. 2003 Reid & Silverstein 1990, ApJ 361, 483 41 clockwise 33 counterclockwise Assume B φ >> B r or B z

8 Observational tracers of magnetic fields perpendicular field in 2 or 3 kpc Polarization of starlight: perpendicular field in 2 or 3 kpc orientation // B ⊥ ------------- 9000 stars parallel field, in situ (masers, clouds) Zeeman splitting : parallel field, in situ (masers, clouds) △ ∝ B // ------ 30 masers perpendicular field Polarization at infrared, mm : perpendicular field orientation // B ⊥ ------------- star formation regions vertical field structures (added) Synchrotron radiation : vertical field structures (added) total intensity S ∝ B ⊥ 2/7, p% ∝ B ⊥ u 2 / B ⊥ t 2 parallel field, integrated (the halo & disk) Faraday rotation: parallel field, integrated (the halo & disk) RM ∝ ∫ n e B // ds ------ 500 pulsars + >1000 EGSes Magnetic field around GC Comparison of magnetic fields of nearby Galaxies to our owns

9 Polarization at mm, sub-mm, infrared Working toward measure B-field of galactic scale thermal emission (of dusts) aligned by B-field in the clouds Hildebrand et al. PASP 112, 1215

10 Poloidal & Toroidal fields near GC Large-scale Toroidal fields permeated in the central molecular zone (170pc*30pc) (170pc*30pc) sub-mm obs of p% toroidal field directions determined by averaged RMs of plumes or SNR! Poloidal field filaments Unique to GC --- dipolar geometry!? (Yusef-Zadeh et al., 1984;1997 Morris 1994; Lang et al.1999) (after Novak et al. 2003) 150pc GC Predicted B-direction

11 near GC Magnetic fields in our Galaxy: near GC Spiral arms to centre: continue near GC? – Yes in NGC 2997 (Han et al. 1999) –- How strong? Do not know! Poloidal fields: – reason for jets? – dipole field? – related to vertical-B? – how strong? (from B.D.C. Chandran 2000)

12 transverse B-structures Synchrotron radiation: transverse B-structures Global B-field structure from linearly polarized emission RM maps helps on directions of (disk &) halo field! MPIFR has a group working on this for 25 years! No information of B-directions! Han et al. 1999, A&A 384, 405 Two Possible origin of polarization: Large-scale magnetic field as vectors shown (convention) Large-scale magnetic field as vectors shown (convention) Anisotropic random field compressed by large-scale density wave Anisotropic random field compressed by large-scale density wave

13 Observational tracers of magnetic fields perpendicular field in 2 or 3 kpc Polarization of starlight: perpendicular field in 2 or 3 kpc orientation // B ⊥ ------------- 9000 stars parallel field, in situ (masers, clouds) Zeeman splitting : parallel field, in situ (masers, clouds) △ ∝ B // ------ 30 masers perpendicular field Polarization at infrared, mm : perpendicular field orientation // B ⊥ ------------- star formation regions vertical field structures (added) Synchrotron radiation : vertical field structures (added) total intensity S ∝ B ⊥ 2/7, p% ∝ B ⊥ u 2 / B ⊥ t 2 parallel field, integrated (the halo & disk) Faraday rotation: parallel field, integrated (the halo & disk) RM ∝ ∫ n e B // ds ------ 550 pulsars + >2000 EGSes

14 Pulsars: Uique probes for Large-scale Galactic B-field Widely distributed in Galaxy Widely distributed in Galaxy Distance from DM: 3-D B-field Distance from DM: 3-D B-field Linearly polarized: RM easy to obs Linearly polarized: RM easy to obs No intrinsic RMs: Direct No intrinsic RMs: Direct Pulsar distribution

15 Why? Pulsars as probes for Galactic B-field Polarized. Widely spread in our Galaxy. Faraday rotation: Distances estimated from pulse dispersion: » <=== » <=== the delay tells DM » » the rotation of position ===> » angles tells RM value ===> » Average field strength is

16 Knowledge of 10 years ago ……

17 disk field: which one? disk field: * 3 models * which one? Concentric Rings Axi-symmetric Bi-Symmetric Spiral Rings model spiral (ASS) (BSS) Galactic magnetic fields: 10 years ago Halo field: no idea on halo field Poloidal fieldsnear GC: Yes see nonthermal filaments Halo field: * no idea on halo field * Poloidal fields near GC: Yes see nonthermal filaments

18 Axi-Symmetric Spiral model by J.P. Vallee Main Problem: fields go across the arms Just one radius range for reversed fields Just one radius range for reversed fields Not consistent with field reversals near ?? -- Perseus arm?? the Norma arm !! -- the Norma arm !! BSS reversal ? ?

19 Ring model: Concentric rings of reversed fields Selection effect problem ?? Selection effect problem ?? Field lines go across the arms? Field lines go across the arms? Inconsistent Formula for the BSS when modeling ?? Inconsistent Formula for the BSS when modeling ?? It is the zero-order modelling only for azimuthal magnetic field ! by R. Rand & S. Kulkarni (1989) R. Rand & A.Lyne(1994) There were not as many pulsar RMs as today….

20 Bi-Symmetric Spiral Model Proposed from RMs of Extragalactic Radio Sources: Simard-Normandin & Kronberg (1980) Sofue & Fujimoto (1983) Confirmed by Pulsar RMs: Han & Qiao (1994) Indrani & Deshpande (1998) Han, Manchester, Qiao (1999) Han,Manchester, Lyne, Qiao(2002) Supported by starlight polarization Heiles (1996) The best match to all evidence field reversals & pitch angle – 8°±2° ? ? ( the field stronger in interarm region ? ? )

21 Galactic B-Field : 10 years ago SunGalactic center Disk field: A few kpc! Center: Poloidal field 3 models: which ? Halo field : no idea ! 30kpc

22 Current knowledge …… Central field & halo fieldCentral field & halo field disk field:disk field: directions & Strength directions & Strength magnetic energy spectrummagnetic energy spectrum

23 Poloidal & Toroidal fields near GC Toroidal fields (Novak et al. 2003, 2000) permeated in the central molecular zone central molecular zone (400pc*50pc) (400pc*50pc) sub-mm obs of p% toroidal field directions determined by averaged RMs of plumes or SNR! Poloidal field filaments Unique to GC --- dipolar geometry! (Morris 1994; Lang et al.1999) (from Novak et al. 2003) 150pc GC Predicted B-direction

24 near GC Magnetic fields in our Galaxy: near GC Spiral arms & B- fields continue near GC? – Yes in NGC 2997 (Han et al. 1999) –- How strong? Poloidal fields – reason for jets? – dipole field? – related to vertical-B? – how strong? (from B.D.C. Chandran 2000)

25 unique to our Galaxy To study halo field: unique to our Galaxy The largest edge-on Galaxy in the sky Pulsars and extragalactic radio sources as probes Pulsars RM distribution

26 The largest edge-on Galaxy in the sky Pulsars and extragalactic radio sources as probes Extragalactic Radio Sources RM distribution unique to our Galaxy To study halo field: unique to our Galaxy away from us RM<0 RM>0 to us

27 Anti-symmetric RM sky: A0 dynamo (Han et al. 1997 A&A322, 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 A0 dynamo The first dynamo mode identified on galactic scalesThe first dynamo mode identified on galactic scales Bv

28 Unpublished database ……EGRes

29 Magnetic field configurations for basic dynamos M31 : only 21 polarized bright background sources available !! Han, Beck, Berkhuijsen (1998): An even mode (S0) dynamo may operate in M31 ! A0 S0 S1

30 RMs of EGRs for the halo B-field Only about 1000 RMs available in literature upto now... We are using Effelsberg -100m telescope to make a RM survey of 1700 sources, enlarge the cover density by a factor of three in most sky area……

31 Current knowledge …… Central field & halo fieldCentral field & halo field disk field:disk field: »directions »Strength magnetic energy spectrummagnetic energy spectrum

32 (Han et al. 2005, to be submitted) Pulsar RM distribution in Galactic plane Red: new measurements by Parkes 64m telescope (Han et al. 2005, to be submitted)

33 Pulsar RM distribution in Galactic plane red: new measurements by Parkes 64m telescope

34 CCW B-field along the Norma arm: from New Pulsar RMs possible field directions Field directions newly determined Han et al. 2002, ApJ 570, L17 B-field directions Coherent B-field directions >5 kpc along Norma arm large-scale Another reversed field in large-scale? ??

35 (Han et al. 2005, to be submitted) Pulsar RM distribution in Galactic plane red: new measurements by Parkes 64m telescope (Han et al. 2005, to be submitted)

36 (Han et al. 2005, to be submitted) Large-scale magnetic field in the Galactic disk (Han et al. 2005, to be submitted)

37 always counterclockwise in arm region! always counterclockwise in arm region! clockwise in interarm region ? clockwise in interarm region ? Different from previous models ! Tight BSS ? Different from previous models ! Tight BSS ? More data still needed! More data still needed! Weisberg et al. 2004: large-scale magnetic fields lies in arm region?! Yes! (Han et al. 2005, to be submitted) Large-scale magnetic field in the Galactic disk (Han et al. 2005, to be submitted)

38 Current knowledge …… Central field & halo fieldCentral field & halo field disk field:disk field: »directions »Strength magnetic energy spectrummagnetic energy spectrum

39 Radial dependence of regular field strength (Han et al. 2005, to be submitted)

40

41 Current knowledge …… Central field & halo fieldCentral field & halo field disk field:disk field: directions & Strength directions & Strength magnetic energy spectrummagnetic energy spectrum

42 Why our Galaxy has magnetic field? Probably Dynamo! How dynamo works? Alpha-Omega effect. Dynamo Really works? Computer Simulations …. Computer Simulations ….

43 Many Simulations of dynamos ---- check spacial B-energy spectrum & its evolution e.g. Magnetic energy distribution on different spatial scales (k=1/λ) e.g. Magnetic energy distribution on different spatial scales (k=1/λ) Many papers by N.E. L. Haugen, A. Brandenburg, W. Dobler, ….. N.E. L. Haugen, A. Brandenburg, W. Dobler, ….. A. Schekochihin, S.C. Cowley, S. Taylor, J. Moron, ….. A. Schekochihin, S.C. Cowley, S. Taylor, J. Moron, ….. E. Blackman, J. Maron ….. E. Blackman, J. Maron ….. Others ….. Others ….. No real measurements No real measurements to check whether to check whether dynamo works or not! Far away from telling anything about a real galaxy …… Don’t know much about the large-scale magnetic field...

44 What spatial magnetic energy spectrum does our Galaxy have?

45 Spatial fluctuation spectrum for electron density “The Big Powerlaw in the Sky ” B-field & electrons coupling? If so, B-energy spectrum? Kolmogorov over 12 orders in scale? 10 pc 1000 km (Armstrong, Rickett & Spangler 1995)

46 Minter & Spangler 1996 Previously only available information from RM structure function Spatial energy spectrum of B Previously only available information from RM structure function λ< ~4pc: consistent to Kolmogorov 3D 80>λ> ~4pc: turbulence in 2D?

47 Pulsar RM distribution in Galactic plane red: new measurements by Parkes 64m telescope

48 Spatial magnetic energy spectrum of our Galaxy (Han et al. 2004, ApJ 610, 820) Minter & Spangler 1996 By pulsar RM/DM Email from A. Minter

49 We now can tell about ---- Global structure of Galactic magnetic field Halo field structure Disk field structure

50 Galactic B-Field : 10 years ago SunGalactic center Disk field: A few kpc! Center: Poloidal field 3 models: which ? Halo field : no idea ! 30kpc

51 Spatial Energy spectrum Radial dependenceRadial dependence Conclusive Remarks: More data needed -- Pulsars are unique powerful probes Halo field Disk field

52 If I have time, I tell you more about what we are doing …… Thanks for your attention.

53 Field reversals exterior to the Perseus arm -- it is fine! Brown et al. 2003, ApJ 593, L29 Mitra et al. 2003, A&A 398,993 Han et al. 1999 Lyne & Smith 1989 Evidence at 150<l<100 is very weak, but Evidence for two reversals at l~70 is hard!

54 Difference for RMs of PSRs & EGRes

55 Rainer Beck: Rainer Beck: Unique measurement of Vertical B-component Bv = 0.2 ~ 0.3  G pointing from SGP to NGP (Effect of the NPS discounted already!) Local vertical components: from poloidal field? South Galactic Pole North Galactic Pole (see Han & Qiao 1994; Han et al. 1999)


Download ppt "Magnetic fields in our Galaxy JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China Thanks for cooperation."

Similar presentations


Ads by Google