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Magnetic Fields in Star Formation Alyssa A. Goodman Harvard-Smithsonian Center for Astrophysics Tyler Bourke Smithsonian Astrophysical Observatory/SMA Figure credit: Heitsch et al. 2001 simulation
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Question 1: How Much Do Magnetic Fields Matter in Molecular Clouds? see Bourke et al. 2001; Crutcher 1999 and references therein
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Question 2: How, Exactly, Do Magnetic Fields Matter in the Disk/Outflow System? figure from Ostriker & Shu 1998 figure courtesy NASA
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B-Observers Toolkit Neutral ISM Polarimetry Background Starlight Thermal Emission Zeeman Thermal Emission Absorption Masers Polarized Spectral Lines Ionized ISM Polarized continuum B direction Faraday Rotation B=RM/DM Recombination Line Masers
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Large Molecular Clouds Jets and Disks "Cores" and Outflows Solar System Formation Which Polarimetry Where Background Starlight nothing yet... Thermal Emission & Scattered Light but not inside cold, dark clouds
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Large Molecular Clouds Jets and Disks "Cores" and Outflows Solar System Formation Which Zeeman Where H I, including self-absorption, OH nothing yet... OH and CN in Cores H 2 O and OH Maser Emission
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Large Molecular Clouds Jets and Disks "Cores" and Outflows Solar System Formation Polarized (Thermal) Spectral Lines CO detected at BIMA & JCMT nothing yet… nothing yet...nothing yet… NEW!
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B-Analysis Toolkit Analytic Predictions Numerical Simulations Chandrasekhar-Fermi Method
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Naïveté or the Simplest Analytic Models: The way we once thought polarization maps might look…
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Magnetohydrodynamic Models Strong Field =0.01, M =7 Weak Field =1, M =7 Synthetic Polarization Maps from Ostriker, Stone & Gammie 2001; see also Heitsch et al. 2001; Padoan et al. 2003
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The Chandrasekhar-Fermi Method see Myers & Goodman 1991; Sandstrom & Goodman 2003 for details ~modeling field strength from polarization map messiness messy weak field ordered strong field Simulations often imply N corr ~4 in “dark clouds” Polarization Maps Spectral-line maps Extinction, dust emission, or spectral-line maps
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B-Observers Toolkit Neutral ISM Polarimetry Background Starlight Thermal Emission Zeeman Thermal Emission Absorption Masers Polarized Spectral Lines
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The Galaxy Serkowski, Mathewson & Ford, et al. Note: Background starlight polarization is parallel to l.o.s. field
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Dark Cloud Complexes: 1-10 pc scales
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Polarization of Background Starlight in Taurus
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Magnetic Fields Dark Cloud Complexes: 1-10 pc scales
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Background Starlight Polarimetry “Fails” at A V >1.3 mag in Dark Clouds 3.0 2.5 2.0 1.5 1.0 0.5 0.0 P R [%] 43210 43210 A V [mag] Background to Cold Dark Cloud Arce et al. 1998 Background to General ISM cf. Goodman et al. 1992; 1995 “Bad Grains” in Cold Cloud Interiors
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Thermal Emission Polarimetry 10 -20 10 -18 10 -16 10 -14 10 -12 10 -10 10 -8 B [erg sec cm -2 Hz ster ] 0.0010.010.1110100 Wavelength [cm] 10 8 9 11 10 12 10 13 10 14 Frequency [Hz] Emissivity-Weighted, normalized, blackbodies 10 K30 K 100 K sub-mm: JCMT, CSO SMA far-IR:KAOSOFIA mm: OVRO, BIMA, CARMA ALMA
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Thermal Emission Results Summary >pc-scales: No earthbound instrument sensitive enough, no space instrument capable (a shame!) ~pc-scales: KAO/STOKES, CSO/HERTZ, JCMT/SCUBA have all had success, and all see “polarization holes” at high density (see Brenda Matthews’ talk!) <<pc scales: BIMA & OVRO have had success, and also see “polarization holes” at high density Honestly: Results from all scales suggestive, but not yet “conclusive,” on field’s role at large or small scales. CF method promising.
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Vallé et al. 2003 “Polarization Hole”
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W51 Polarization from BIMA: Lai et al. 2001 “Polarization Holes”
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How to Interpret Maps with “Holes”? Padoan, Goodman, Draine, Juvela,Nordlund, Rögnvaldsson 2001 3-D simulation super-sonic super-Alfvénic self-gravitating Model A: Uniform grain- alignment efficiency
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Padoan, Goodman, Draine, Juvela,Nordlund, Rögnvaldsson 2001 3-D simulation super-sonic super-Alfvénic self-gravitating Model B: Poor Alignment at A V ≥3 mag How to Interpret Maps with “Holes”?
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SCUBA-like Cores with Holes Padoan, Goodman, Draine, Juvela,Nordlund, Rögnvaldsson 2001
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It seems nearly all polarization maps show decrease in polarizing efficiency with density. Derived models of 3D field (for comparisons) need to take this into account.
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Zeeman Results Summary see Bourke et al. 2001; Crutcher 1999 and references therein Detections hard to come by In general, B less than or “close” to equipartition
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The Chandrasekhar-Fermi Method with correction factors suggested by simulations, agrees well with Zeeman data, but is MUCH easier to use Sandstrom & Goodman 2003 Shown here for optical polarization, in dark clouds, but seems to work (compare well with measured Zeeman) for emission polarization as well.
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Polarized Spectral-Line Summary Effect predicted by Goldreich & Kylafis, 1981 1st detection in a star-forming region (NGC 1333): Girart et al. 1999 (BIMA) Subsequent detection with JCMT/SCUBA (in NGC2024): Greaves et al. 2001 Still very difficult to interpret (polarization can be parallel or perpendicular to B!--need context)
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NGC 1333 IRAS 4A Girart et al. 1999 CO Polarization Dust Polarization (in white)
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“Not, Exactly”
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B-Analysis “Challenges” Line of sight averaging of vector quantity=complex radiative transfer Decline of grain alignment efficiency in high- density regions (how to interpret data w/holes?) Multiple velocity components in spectral lines (particularly bad in Zeeman case) Ambiguities in interpreting polarized spectral- line emission (depends on , etc.)
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Question 1: How Much Do Magnetic Fields Matter in Molecular Clouds? Question 2: How, Exactly, Do Magnetic Fields Matter in the Disk/Outflow System?
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The High-Resolution Future: Observations SMA, CARMA, ALMA (~Question 2) Resolve field in circumstellar disks & flows near YSOs Dust continuum polarimetry (see Matthews) mm spectral-line polarimetry (see Greaves/Crutcher who’s there?) Square Kilometer Array (~Question 1) Understand field-tangling/structure within big single- dish beams Zeeman observations (see Bourke) RM/DM & synchrotron observations (see Gaensler) Connect our views of the field in neutral & ionized ISM?? Remember…1 arcsec = 100 A.U. at 100 pc
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The High-Resolution Future: Theory & Simulation Analytical Detailed predictions of the (about-to-be-observed) interface between the stellar and disk/outflow (e.g. “X-wind”) field structure (Question 2) Numerical (near-term) Models of synthetic polarization and Zeeman observations at ~100 A.U. scales (Question 2) (longer-term) High-resolution MHD simulation all the way from pc to A.U. scales (Questions 1& 2) (Current limits ~10 pc to 0.1 pc) 10 9 3D pixels gives resolution of ~10 A.U. over a volume of 0.1 pc
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The Unconventional Future Incorporating neutral/ion line width ratios to get 3D field (see Houdé et al. 2002) Anisotropy in velocity centroid maps as a diagnostic of the mean magnetic field strength in cores (see Vestuto, Ostriker & Stone 2003) Interpretation of microwave polarization (e.g. from WMAP) as due to rapidly spinning (magnetically aligned?) grains (see Finkbeiner 2003 and Hildebrand & Kirby 2003 & references therein)
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Polarization vs. Intensity Padoan, Goodman, Draine, Juvela,Nordlund, Rögnvaldsson 2001
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Effects of Viewing Angle x y z Uniform Alignment No Alignment A V >3
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The Way Numerical Models say it Is…
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Polarization of Background Starlight
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Polarization of Thermal Dust Emission
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(Sample) SCUBA Polarimetry of Dense Cores & Globules Does polarization map give true field structure? Polarization drops with sub- mm flux (similar to p decreasing with A V ) Plots and data from Henning, Wolf, Launhart & Waters 2001
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2" resolution; Lai et al. 2002
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