Star Formation on Galactic Scales

Star Formation on Galactic Scales

Star Formation on Galactic Scales Petchara Pattarakijwanich Princeton University 15 January 2013 Outline I Observation method overview. I How to measure star formation rate (SFR). I How to measure gas density in various phases. I Observational results. I Disk-averaged. I Spatially-resolved. I Theoretical efforts. Empirical Relations I A few empirical relations are found to fit the data well. N I ΣSFR = AΣgas (Kennicutt & Schmidt Law) Σgas I ΣSFR = A tdyn I ΣSFR / ηPtotal I How do we measure these quantities? Measuring Gas Density I Atomic Gas. I HI spin-flip hyperfine transition. I λ = 21cm, ν = 1:42GHz R 5 DL 2 Fν dv I M = 2:343 × 10 M (1 + z)( ) ( ) HI Mpc Jy km s−1 I Molecular Gas. I H2 does not emit strongly. I Use other trace molecules, most commonly CO. −2 N(H2) 20 1=2 5:5K=Texc cm I XCO = R = 1:58 × 10 n (e ) −1 TAdv 3 K km s I Various issues: I CO line is optically thick I XCO varying. Why does H2 not emit strongly? I Common interpretation: Lack of electric dipole. I Actually: Small moment of inertia ! Large energy gap ! Not populated. I mass ∼ 15 times smaller, size ∼ 50% smaller. 2 J(J+1)~ I E = 2I where I = µr 2. http://hyperphysics.phy-astr.gsu.ed Measuring Star Formation Rate I Various ways, each have different issues and are sensitive to different timescales. I Star count. I Ultraviolet. I Emission lines. I Infrared. I X-ray. I Radio. Measuring Star Formation Rate: Star-count I With complete data of individual stars in a group and good stellar evolution model, one can model everything. Mu _ P I hM∗i = N(M∗; t∗)M∗=t∗ M∗=Ml I Problems: I Need very high quality data. I Resolution limit. Not possible outside local group. Measuring Star Formation Rate: UV & IR I UV I Emitted by young stars. I Main database is GALEX. I Issue: Dust. I IR I Emitted by dust cloud surrounding young stars I Various database (WISE, Spitzer, Herschel, Planck) I Issue: Lack of dust. I Complementary to each other. Measuring Star Formation Rate: Emission Lines I Emission lines are associated with HII regions. I Commonly used lines: I Hα (Line of choice). I [OII]λ3727. I Lyα. I Paschen Series. I metal IR cooling lines. I Problems: I Dust. I Calibration. Measuring Star Formation Rate: X-ray & Radio I Both X-ray and radio emissions are associated with young phase of stellar evolution. I X-ray: X-ray binary, supernovae & remnants, young stars. I Radio: free-free from HII region, synchrotron from supernova remnants. I Problem: AGNs also emit X-ray and radio wave. Measuring Star Formation Rate: Combination Kennicutt & Evans (2012) Measuring Star Formation Rate: Calibration Kennicutt & Evans (2012) Observables ! Theoretical Quantities Leroy et al (2008) Observational Results I Apply these methods to measure real galaxies. I Empirical correlations: 1:4 I ΣSFR / Σgas (Kennicutt & Schmidt Law) Σgas I ΣSFR / tdyn I ΣSFR / ηPtotal I Constrains for theories and high-resolution simulations. I Used as \subgrid" model for low-resolution simulations. Observational Results Reviews I This starts with the prediction by Schmidt (1959) and observation by Kennicutt (1998). The so-called Kennicutt-Schmidt Law. Kennicutt (1998) More modern dataset I This game can be played with large galaxy sample. I Various types and selection methods. I The correlation still holds. Kennicutt & Evans (2012) Resolved KS law I One can also do this with resolved data. I Either point-by-point basis, or ring-averaged. I Some complications on small scale. Kennicutt & Evans (2012) Resolved KS law at high redshift I Similar result for galaxies at redshift z ∼ 1 from recent paper. Freundlich et al (2013) −2 Break in KS law at Σgas = 10M pc I Break from N ∼ 1:4 at −2 Σgas ∼ 10M pc I Some papers argue that this is associated with gravitational instability scale. However this is not likely the case considering the radial profile. I This is more likely the sign of second parameter. ΣSFR can take any value −2 for Σgas ∼ 10M pc Leroy et al (2008) −2 Break in KS law at Σgas = 10M pc I The correlation with Σmol −2 remains below 10M pc . I This indicates varying fraction of molecular and atomic gas, as well as the relative importance of gas and stellar potential. Leroy et al (2013) Theoretical aspects I Challenges for Theorists: I Explain the form of empirical relations. I Explain the generally low SFR. I Naive expectation Σgas would be ΣSFR ∼ tff and this would lead to 2 orders of magnitude higher in SFR. Kennicutt (1998) Stellar Feedback I Sources of feedback: protostellar jets, stellar winds, supernovae and radiation pressure from young star. I Momentum feedback seems necessary, or the energy is just radiated away easily. I Hopkins et al (2011) implemented this momentum feedback in simulation and showed that it suppress SF. Hopkins, Quataert & Murray (2011) Stellar Feedback Hopkins, Quataert & Murray (2011) Turbulence I Krumholz & McKee (2005) proposed that turbulence-regulated SF can work. This theory is derived from first principle and is based on a few natural assumptions. I Clouds are virialized and supersonically turbulent. I Density distribution is log-normal. I SF happens in dense enough region where gravity is stronger than turbulence. I Predict the empirical relations found from observation. I Does not specify the source of turbulence. This turbulence can be due to feedback. Turbulence Krumholz & McKee (2005) Star Formation as Demand I Traditional thinking: Star formation responds to supply. I Gas is the fuel, it collapses and forms stars. I Only a few percent of GMC mass is turned into stars. I Star formation is very inefficient. I New way proposed by Ostriker, McKee & Leroy (2010): Star formation responds to demand. I In order to keep ISM in equilibrium, energy and turbulence dissipated must be replenished. And pressure must be provided to counter gravity. I Star formation is responsible for these processes. I To sustain this with a few percent rate, star formation is actually very efficient. Star Formation as Demand I A few things have to be balanced I Heating vs. Energy loss via radiation. I Momentum injection vs. Turbulence dissipation. I Pressure vs. Gravity. Kim, Kim & Ostriker (2011) Conclusions I One can learn a lot about galaxies with right measurements. I Star formation rate in galaxies follows certain empirical relationships. I These observational results can be used as a test for theories or input for simulations. I Theories are being developed to explain these observations. None of them is complete yet. But with better dataset, simulations and theories the understanding of this process is advancing quickly. Reference I Bigiel et al (2008) \The Star Formation Law in Nearby Galaxies on Sub-Kpc Scales", AJ, 136, 2846 I Freundlich et al (2013) \Towards a resolved Kennicutt-Schmidt law at high redshift", arXiv:1301.0628 I Hopkins, Quataert & Murray (2011) \Self-regulated star formation in galaxies via momentum input from massive stars", MNRAS, 417, 950 I Kennicutt (1998) \The Global Schmidt Law in Star-forming Galaxies", ApJ, 498, 541 I Kennicutt & Evans (2012) \Star Formation in the Milky Way and Nearby Galaxies", ARA&A, 50, 531 I Kim, Kim & Ostriker (2011) \Regulation of Star Formation Rates in Multiphase Galactic Disks: Numerical Tests of the Thermal/Dynamical Equilibrium Model", ApJ, 743, 25K I Krumholz & McKee (2005) \A General Theory of Turbulence-regulated Star Formation, from Spirals to Ultraluminous Infrared Galaxies", ApJ, 630, 250 I Leroy et al (2008) \The Star Formation Efficiency in Nearby Galaxies: Measuring Where Gas Forms Stars Effectively”, AJ, 136, 2782 I Leroy et al (2013) \Molecular Gas and Star Formation in Nearby Disk Galaxies", arXiv:1301.2328 I Ostriker, McKee & Leroy (2010) \Regulation of Star Formation Rates in Multiphase Galactic Disks: A Thermal/Dynamical Equilibrium Model", ApJ, 721, 975O.

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