Galactic-Scale Winds. J. Xavier Prochaska Inster(stellar+galactic) Medium Program of Studies [IMPS] UCO, UC Santa Cruz.

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1 Galactic-Scale Winds JXP, Kasen, Rubin, ApJ, to be submitted J. Xavier Prochaska Inster(stellar+galactic) Medium Program of Studies [IMPS] UCO, UC Santa Cruz Kate Rubin (IMPS, MPIA) Dan Kasen (UCSC, UCB/LBL) 1

2 Feedback 2

3 Feedback ADS Search: Refereed, 2010, feedback or wind 2

4 Cool Gas Outflows Blue-shifted absorption reveals outflowing material Weiner+09 (see Koo s talk tomorrow?) Set by [OII] emission 3

5 Cool Gas Outflows Blue-shifted absorption reveals outflowing material Tremonti+08, Weiner+09, Rubin+09 Rupke+05, Martin06, Chen+10 Steidel+96 Lowenthal+97 Pettini+02 Steidel+10 4

6 The Great Unknowns SF Galaxy Earth 5

7 The Great Unknowns Distance (dwind) SF Galaxy Earth 5

8 The Great Unknowns Distance (dwind) Near (e.g. 100 pc)? SF Galaxy Earth 5

9 The Great Unknowns Distance (dwind) Near (e.g. 100 pc)? Far (e.g. 10 kpc)? SF Galaxy Earth 5

10 The Great Unknowns Distance (dwind) Near (e.g. 100 pc)? Far (e.g. 10 kpc)? Near and Far? SF Galaxy Earth 5

11 The Great Unknowns Distance (dwind) Near (e.g. 100 pc)? Far (e.g. 10 kpc)? Near and Far? Extremely far!! (see Rubin+10, ApJ, 712, 547) z=0.43 z=0.67 5

12 The Great Unknowns Distance (dwind) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Earth SF Galaxy 6

13 The Great Unknowns Distance (dwind) Distribution (Ω) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Earth SF Galaxy 6

14 The Great Unknowns Distance (dwind) Distribution (Ω) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Earth SF Galaxy 6

15 The Great Unknowns Distance (dwind) Distribution (Ω) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Earth SF Galaxy 6

16 The Great Unknowns Distance (dwind) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Distribution (Ω) Isotropic? Earth SF Galaxy 6

17 The Great Unknowns Distance (dwind) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Distribution (Ω) Isotropic? Conical? Earth SF Galaxy 6

18 The Great Unknowns Distance (dwind) Near (e.g. 100 pc) Far (e.g. 10 kpc) Near and Far Distribution (Ω) Isotropic? Conical? Highly asymmetric? Earth SF Galaxy 6

19 The Greater Unknowns Earth SF Galaxy 7

20 The Greater Unknowns Mass flux (of the wind) M w Ω d wind v wind Earth SF Galaxy 7

21 The Greater Unknowns Mass flux (of the wind) Power (of the wind) M w Ω d wind v wind Ė M w vwind 2 Earth SF Galaxy 7

22 The Greater Unknowns Mass flux (of the wind) Power (of the wind) M w Ω d wind v wind Ė M w vwind 2 Momentum (of the wind) P M w v wind Earth SF Galaxy 7

23 The Greater Unknowns Mass flux (of the wind) Power (of the wind) M w Ω d wind v wind Ė M w vwind 2 Momentum (of the wind) P M w v wind What drives the flow? Earth SF Galaxy 7

24 The Greater Unknowns Mass flux (of the wind) Power (of the wind) M w Ω d wind v wind Ė M w vwind 2 Momentum (of the wind) P M w v wind What drives the flow? What is its age? Earth SF Galaxy 7

25 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind Earth 8

26 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

27 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

28 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

29 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

30 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

31 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

32 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

33 P-Cygni (Cartoon) Canonical absorption+emission profile of a wind 1D Spectrum for MgII 2796 Earth 8

34 (Idealized) Cool Gas Outflow Models Inspired by the Rubin et al. observations that follow Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 9

35 (Idealized) Cool Gas Outflow Models Inspired by the Rubin et al. observations that follow Radiative Transfer Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 9

36 Wind Profile (Fiducial Model) The key quantity is the optical depth profile Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 10

37 Wind Profile (Fiducial Model) The key quantity is the optical depth profile v ~ r n ~ r -2 Include metals Isotropic and dust-free Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 10

38 MgII Profiles (Fiducial Model) Standard P-Cygni profiles 11

39 MgII Profiles (Fiducial Model) Standard P-Cygni profiles 11

40 MgII Profiles (Fiducial Model) Standard P-Cygni profiles Absorption at dv >~ -200 km/s has been filled-in 11

41 MgII Profiles (Fiducial Model) Standard P-Cygni profiles Absorption at dv >~ -200 km/s has been filled-in Standard analysis would (i) require partial covering of the source, (ii) recover the wrong optical depth, and (iii) miss gas at v~0 km/s 11

42 Wind Emission (Fiducial Model) Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

43 Wind Emission (Fiducial Model) Consider the surface brightness of observed flux Scattered photons And, of course, the source Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

44 Wind Emission (Fiducial Model) Consider the surface brightness of observed flux Scattered photons And, of course, the source Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

45 Wind Emission (Fiducial Model) Consider the surface brightness of observed flux Scattered photons And, of course, the source At v=-100 km/s, all of the emission is scattered photons From the front side of the wind Concentrated near the source But, extending to edge of the wind Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

46 Wind Emission (Fiducial Model) Consider the surface brightness of observed flux Scattered photons And, of course, the source At v=-100 km/s, all of the emission is scattered photons From the front side of the wind Concentrated near the source But, extending to edge of the wind At larger velocities, the source dominates But scattered photons from the backside of the wind contribute Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

47 Wind Emission (Fiducial Model) Consider the surface brightness of observed flux Scattered photons And, of course, the source At v=-100 km/s, all of the emission is scattered photons From the front side of the wind Concentrated near the source But, extending to edge of the wind At larger velocities, the source dominates But scattered photons from the backside of the wind contribute Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 12

48 FeII Transitions 13

49 FeII Transitions Resonant lines Fluorescence (FeII*) UV pumping 13

50 FeII Profiles (Fiducial Model) FeII 2600 shows a P-Cygni like profile FeII 2586 absorption is emitted as FeII* 2612,2632 Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 14

51 FeII* Emission (Fiducial Model) 15

52 FeII* Emission (Fiducial Model) Similar to MgII emission, but nearly symmetric about v=0km/s 15

53 Radiative Transfer: Key Implications Line-emission is a generic prediction Total equivalent width is roughly zero Every absorbed photon is re-emitted Even for dusty, non-isotropic winds Not shown in this talk (trust/ask me) Scattered photons can significantly alter absorption profiles Mis-interpret as partial covering, lower optical depth, etc. Insensitive to gas at v ~ 0 km/s (infall?) Be *especially* wary of stacked spectra Scattered photons offer an additional (more powerful?) probe of winds Size, Morphology, Kinematics Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 16

54 The Real Universe Theoretical wind models are nice and make pretty pictures, but do they even remotely reflect the real Universe? Disclaimer: The study I just described was post-diction (not prediction) Rubin, Prochaska, Menard, Murray, Kasen, Koo, Phillips, 2010, ApJL, submitted 17

55 The Real Universe Theoretical wind models are nice and make pretty pictures, but do they even remotely reflect the real Universe? Disclaimer: The study I just described was post-diction (not prediction) Rubin, Prochaska, Menard, Murray, Kasen, Koo, Phillips, 2010, ApJL, submitted 17

56 The Galaxy (Image) B = 21.7 Bluest of the blue cloud SFR ~ 80 M /yr weak [NeV] 3426 emission (AGN host) ~5 h -1 kpc Rubin+10, ApJL, submitted 18

57 The Galaxy (1D Spectrum) Star-forming galaxy with blue-shifted absorption lines (FeII, MgII) and nebular emission lines (e.g. [OII], Hb, etc.) Rubin+10, ApJL, submitted 19

58 The Galaxy (Velocity Plots) 2 Rubin et al. Fig. 1. The Mg II line profile in the galaxy spectrum. Dotted portions of the spectrum are repeated in the two panels. The systemic velocity is marked with vertical dotted lines. The profile exhibits blueshifted absorption extending to 800 km s 1 relative to the systemic velocity. Emission at and redward of systemic velocity is also evident. Together, these features exhibit apcygni profile, suggestive of a galactic outflow. We propose that the red and blue sections of the spectrum in the left-hand panel arise from different areas of the outflow, as indicated in Figure 4. MgII: P-Cygni profile with strong emission 3. ANALYSIS FeII: Strong resonant-line absorption, modest FeII* emission of 80 M yr 1 state (see 4 andtable1).weproposethattheredandbluesections of the spectrum in the left-hand panel and the magenta.stellarpopulationmodelingindicates and Rubin+10, ApJL, submitted (2010a). We obtained spectroscopy of this galaxy using the Low Resolution Imaging Spectrometer (LRIS) on Keck 1 (Cohen et al. 1994). Our instrumental setup afforded a FWHM resolution ranging between km s 1 and wavelength coverage of Å. We used a 0.9 slitlet oriented NE (see Figure 1 of Rubin et al. 2010a) and collected six 1800 sec exposures with FWHM 0.6 seeing. The data were reduced using the XIDL LowRedux 4 data reduction pipeline. As noted in Rubin et al. (2010a), this galaxy is exceptionally bright for its redshift, with a star formation rate that the spectrum is dominated by light from the intense star formation activity. The deepest parts of the Mg II and Fe II resonance absorption lines are blueshifted by km s 1,withhighvelocitytailsextendingto 800 km s 1,indicatingthattheseionstraceanoutflow (see Figures 1 and 2). Here we analyze the characteristics Fig. 2. Fe II transitions in the galaxy spectrum. The systemic velocity is marked with vertical dotted lines. The left-hand column shows resonance absorption lines, while the right-hand column shows Fe II* emissionprofiles(topfourpanels)andthe[neiii] λ3869 line (bottom panel; black). The green line in the bottom panel shows the coadd of the detected (and unblended) Fe II* emission lines. Gray arrows mark Fe II* transitionsarisingfrom states that cannot be radiatively excited directly from the ground cyan sections in the right-hand panel arise from different areas of the outflow, as indicated in Figure 4. tract a model of the two-dimensional continuum profile from the original two-dimensional spectrum. The residual emission extends up to 2 from the spatial 20

59 The Galaxy (2D Spectrum) Stellar continuum MgII Emission MgII Absorption Rubin+10, ApJL, submitted 21

60 The Galaxy (Subtracted Spectrum) Spatially extended MgII Emission Extended emission detected to ~1, i.e. ~7 h -1 kpc Rubin+10, ApJL, submitted 22

61 The Galaxy (Subtracted Spectrum) Extended emission detected to ~1, i.e. ~7 h -1 kpc Rubin+10, ApJL, submitted 22

62 The Galaxy (Subtracted Spectrum) Extended emission detected to ~1, i.e. ~7 h -1 kpc First direct constraints on the spatial extent of the flow! Rubin+10, ApJL, submitted 22

63 Further Implications LBG winds Steidel+10 wind model is unlikely to reproduce the observations (They ignored scattered photons) Beware of conclusions on the non-existence of gas at v >~ 0 km/s Why do many galaxies only show absorption, not emission? Poor data quality Anisotropic winds Bias in galaxy brightness Dust Prochaska, Kasen, & Rubin, ApJ, (nearly) submitted 23

64 (10) Ly! emission from Future Work Mediu IFU observations Constrain the surface brightness profiles e.g. KCWI, X-Shooter, GMOS Constrain the kinematics of this line-emission Implement RT analysis of realistic galactic-scale winds Distributed sources Multi-phase gas Dust, etc. KCWI DEEP 24

65 Dust (Fiducial Model) 25

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