gas mass conversion factors
play

Gas mass conversion factors Axel Weiss MPIfR Bonn, Germany - PowerPoint PPT Presentation

Gas mass conversion factors Axel Weiss MPIfR Bonn, Germany Hercules team PHIBSS team 1 Motivation Daddi ea 2010 Scoville ea 2016 L 850 /L CO(1-0) =0.8 MW Today we have much better data to reevaluate molecular gas mass conversion


  1. Gas mass conversion factors Axel Weiss MPIfR Bonn, Germany Hercules team PHIBSS team 1

  2. Motivation Daddi ea 2010 Scoville ea 2016 L 850 /L’ CO(1-0) α =0.8 α MW Today we have much better data to reevaluate molecular gas mass conversion factors! (CO SEDs, good dust continuum coverage, information from other lines like CI in larger samples of galaxies) 2

  3. Cold H 2 in action - collisions by H 2 are directly observable ! ‘Hot Boltzmann tail’ Multi-component ISM versus 10 3 cm -3 500-2000K 10 4 cm -3 10 5 cm -3 3

  4. Non-LTE line + dust radiative transfer analysis N(H 2 ) / dv ~ n(H 2 ) δ v/ δ r -1 *[mol]/[H 2 ] => line opacity Parameters: N(H 2 ) = N(H 2 ) / dv dv turb * GDMR => dust opacity Physical M(H 2 ) = Ω s N(H 2 ) H 2 density • kinetic temperature • (Weiss ea 2007) turbulence δ v/ δ r; dv turb ; δ v/ δ r ~ sqrt( n(H 2 ) ) • size of the emission region ( Ω s b ff = π r 0 2 ) • Dust and gas are linked at Chemical several levels: [mol]/[H 2 ] • - dust is background for lines Gas to dust mass ratio (GDMR) • - gas columns from lines linked to dust opacity - Tkin >= 0.5*Tdust Radiation Field: Background CMB + Dust (T dust β λ τ =1 ) • 4

  5. Turbulent ISM Density distribution is log normal Column density for a turbulent ISM (simulation) T kin ~ n(H 2 ) - γ ( hydro sim) low dv turb high dv turb Distribution: n(H 2 ), T kin T dust Ω , [ CI] Numbers: dv turb κ vir GDMR, [CO] e.g. Krumholz & McKee 2005, Goldbaum ea 2016 5

  6. Exponential turbulent Disk Distribution: Σ gas (r) => n(H 2 ) (r) T kin T dust, Ω Numbers: dv turb κ vir chemical params Each component is the result from the turbulence model with <n(H 2 )> , <T kin > and Ω source from the exponential disk distribution 6

  7. Sample and Diagnostics Hercules : local (U) LIRGs 26 galaxies CI for 21 Rosenberg ea 2015 High-z QSOs and SMGs (submm selection, above the MS) z=2.0 – 6.3 6 SBs; 6 QSO hosts CI: 8 e.g Weiss ea 2005, 07 Walter ea 2011 9 High-z MS galaxies 2 comp. (z~2, NIR selection) Log M * = 10.5- 11.8 CI: 4 turb. Daddi ea 2010/15 Tacconi ea 2013 Genzel ea 2015 turb. disk Total 44 (U)LIRG 7

  8. CO conversion factor for the MW Calibration for inner part of the MW ( |2.5| < l < |32.5|) Planck, IRAS (Fixsen ea 1999) (Fixsen ea 1999) 2C: α co = 4.0 +/- 1.1 M sol (K km/s pc 2 ) -1 T: α co = 4.9 +/- 1.9 M sol (K km/s pc 2 ) -1 TD: α co = 4.0 +/- 0.7 M sol (K km/s pc 2 ) -1 X co = 1.9 +/- 0.3 x 10 20 cm -2 ( K km/s) -1 (Incl. He correction) Bolatto ea 2003 8

  9. The conversion factors: (turbulent disk model; preliminary) α CO α CI α 850

  10. Test case GN20 Turbulent Disk model GN20 @ z =4.05 Hodge ea 2015 CO(2-1) Limits on α co from M dyn : 170 µ m α co < 3.3 M sol (K km/s pc 2 ) -1 rest continuum we find: α co : 2.2 +/ -0.8 M sol (K km/s pc 2 ) -1 Radial profile model (example) vs observations 10

  11. Disk sizes for different tracers Turbulent Disk model SMM14011 @ z =2.5 Difference compared to Σ ( H 2 ) implies that ALL conversion factors change with r! 11

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend