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CONSTRAINING GALACTIC INFALL WITH DEUTERIUM OBSERVATIONS

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Presentation on theme: "CONSTRAINING GALACTIC INFALL WITH DEUTERIUM OBSERVATIONS"— Presentation transcript:

1 CONSTRAINING GALACTIC INFALL WITH DEUTERIUM OBSERVATIONS
kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović Tijana Prodanović, University of Novi Sad Brian D. Fields, University of Illinois at Urbana Champaign This is a false-color image of the star AE Aurigae (bright source of light slightly off center of image) embedded in a region of space containing smoke-like filaments of carbon-rich dust grains, a common phenomenon. Such dust might be hiding deuterium, an isotope of hydrogen, and stymieing astronomers' efforts to study star and galaxy formation. The FUSE satellite has surveyed the local deuterium concentration in the galaxy and found far more than expected. Because deuterium is a tracer of star and galaxy evolution, this discovery could radically alter theories about how stars and galaxy form. CONSTRAINING GALACTIC INFALL WITH DEUTERIUM OBSERVATIONS

2 REALLY A STORY ABOUt DEUTERIUM...
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović REALLY A STORY ABOUt DEUTERIUM... Only created in Big Bang (Epstein et al. 1976, Prodanović & Fields 2003) All other processes destroy it Monotonic decline from high to low z Deuterium – a powerful tool in cosmology! Cosmic baryometer! BBN success story Measure of how much gas was processed in stars!

3 kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović BUT NOT SO SIMPLE … Large (factor of 3!) variations of D abundance in local ISM over different lines of sight! Both high and low D abundances found “Resolution” to the problem? (Linsky at al. 2006) Deuterium severely depleted onto dust! Measure lower bound on the “true” D “True” ISM D abundance “True” ISM D = 85% of PRIMORDIAL!? Almost NO GASS was PROCESSED in stars!? recall: stars completely destroy D! Reasonable stellar processing: ISM D = 55% of primordial

4 OR A DEUTERIUM FACELIFT …
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović OR A DEUTERIUM FACELIFT … Deuterium must be replenished somehow INFALL/ACCRETION OF PRISTINE GAS! Eg. High-velocity clouds falling on our Galaxy some with metallicity ~10% Solar little or no dust

5 PRIMORDIAL INFALL Changes things …
kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović PRIMORDIAL INFALL Changes things … Increases ISM D abundance Increases gas content of the Galaxy Dilutes metal content of the Galaxy Turns out: Deuterium and Galactic gas fraction observations powerful constraint of the infall rate M51: Cosmic Whirlpool Credit: S. Beckwith (STScI) Hubble Heritage Team, (STScI/AURA), ESA, NASA Explanation: Follow the handle of the Big Dipper away from the dipper's bowl, until you get to the handle's last bright star. Then, just slide your telescope a little south and west and you might find this stunning pair of interacting galaxies, the 51st entry in Charles Messier's famous catalog. Perhaps the original spiral nebula, the large galaxy with well defined spiral structure is also cataloged as NGC Its spiral arms and dust lanes clearly sweep in front of its companion galaxy (right), NGC The pair are about 31 million light-years distant and officially lie within the boundaries of the small constellation Canes Venatici. Though M51 looks faint and fuzzy in small, earthbound telescopes, this sharpest ever picture of M51 was made in January 2005 with the Advanced Camera for Surveys on board the Hubble Space Telescope.

6 How much infall deuterium needs?
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović How much infall deuterium needs? Build a “keep it simple” model Infall and NO outflow Infall rate proportional to star-formation rate Define gas mass fraction Specify return fraction R – fraction of initiall stellar mass that is returned to ISM (follows from Initiall mass function); eg from Salpeter IMF

7 Results: Infall rate constraint
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović Results: Infall rate constraint D vs. gas fraction Shaded = observations Solution must satisfy both Allowed infall rate Almost balances out star-formation!

8 results: Imf constRaint
kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović results: Imf constRaint At late times D and gas fraction approach minimum values Limiting curves above which no solutions for range of return fractions Allowed only Modern IMFs demand At late times: for a large infall deuterium spending through stellar processing and deuterium replenishing through infall will reach some equilibrium constant value that will depend on alpha and R only, but same will be for a small infall since the all the gas will eventually be exhausted except for some small fraction continuously infalling; similarly for gas mass fraction – for large infall reaches some equilibrium, while for small infall there is no minimum value since gas fraction will go to zero.

9 CONCLUSIONS Local ISM D severely depleted onto dust
kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović CONCLUSIONS Local ISM D severely depleted onto dust Local ISM D abundance could be close to primordial Then … Local D and gas fraction observations demand large infall rate , close to star-formation rate Consistent with hierarchical assembly of galaxies by accretion Modern IMFs demand return fraction R~0.4 , but only marginally consistent with our results Prodanovic & Fields, Journal of Cosmology and Astroparticle Physics, Issue 09, pp. 003(2008)

10 kflajsflj XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović Thank You!

11 Model: details Where D is the deuterium mass fraction defined as:
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović Model: details Where D is the deuterium mass fraction defined as: Taking we get: which we can express in terms of the present gas mass fraction by using:

12 model: details – Return fraction
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović model: details – Return fraction Approximate: Then, define return fraction for each progenitor mass as: To find a global return fraction must specify the IMF: For mass ranges and Salpeter IMF we find return fraction Modern IMFs are flatter in the high-mass regime → more high-mass stars → more ejecta → larger return fractions

13 model: details - envelope
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović model: details - envelope For large infall where For small infall where

14 D vs. Metal yields Freshly synthesized metals SN metal yield
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović D vs. Metal yields Freshly synthesized metals SN metal yield Present reasonable estimates consistent with large or no infall since all curves converge.

15 bbn Abundances: SchraMM PLOT
XV National Conference of Astronomers of Serbia, October 4th 2008 Tijana Prodanović bbn Abundances: SchraMM PLOT Cyburt et al. (2004)


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