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Galaxy Rotation: How we know AS413 10/28/2014 D. Clemens.

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Presentation on theme: "Galaxy Rotation: How we know AS413 10/28/2014 D. Clemens."— Presentation transcript:

1 Galaxy Rotation: How we know AS413 10/28/2014 D. Clemens

2 Outline Ways to detect that galaxies rotate Measuring rotations of external galaxies Our problematic location within the Milky Way Clues from the nearby stars Success from Radio Astronomy: HI Sampling the cold ISM: CO (for H2) Outer Galaxy probes: gas+stars New(er) Milky Way probes: APOGEE, Gaia Mass models, dark matter, galaxy assemblage

3 Evidence that Galaxies Rotate Optical spectroscopy of galaxies – Large-aperture observations reveal absorption lines that are too broad to be from single stars Would imply impossibly high surface gravities Must be due to Doppler shifting of many stars with a range of radial velocities (RVs) wrt us Velocity dispersion of that galaxy (gravitational potential) – Emission lines from large- apertures don’t necessarily trace velocity dispersion Emission regions don’t span galaxy uniformly Elliptical galaxies don’t generally have emission lines Multi-Object or IFU (Integral Field Unit) RV observations – Velocity dispersion from scatter in RVs (MOS) – Velocity dispersion from IFU images

4 http://www.usm.uni-muenchen.de/people/saglia/praktikum/galspectra/node3.html

5 Multi-object fiber-feed – 2dF http://www.2dfquasar.org/Spec_Cat/gfx/2dFpic3.jpg One fiber per galaxy Good for measuring galaxy RVs and cluster RV dispersions

6 Lots of spectra taken simultaneously See atmosphere as well as stellar/galaxy absorptions, emission lines Most in this image are earth’s atmosphere http://astrobites.org/wp-content/uploads/2014/02/MOS.jpg

7 Integral Field Unit (3 types shown) – feeding light to multiple spectrographs Resolve individual galaxies to elucidate RVs http://ifs.wdfiles.com/local--files/what-is-ifs/ifu_designs.jpg

8 All Measure Velocity Dispersions Alternatively – put spectrograph slit along spiral galaxy axis (long axis) – If spiral galaxy shows a long-axis, it has some inclination (no E7 spirals!) – If inclination angle can be deduced (from apparent axis ratio a/b, say), can correct apparent RVs to disk circular velocities – As a function of offset from the galaxy center, too – Holland, Ford, Rubin (1970s)

9 https://www.astro.virginia.edu/class/whittle/astr553/Topic05/t5_rotcurv_rubin.gif

10 Convert wavelength shift to RV, correct for inclination – Mostly due to HII region emission, so spiral arms well-represented – “Fold” curve of velocity vs offset about center Buta,et al. 1987

11 Lots-o-galaxies – similar ‘Rotation Curves’ Rapid rise from center Then flattening http://ned.ipac.caltech.edu/level5/Bothun2/Figures/rcurves.gif

12 Wrong Answer! (or so they/we thought) Add up light from luminous matter (stars) Compute mass enclosed to some radius Predict circular rotations at each radius Too little! Need more matter – dark matter Begeman, Broels and Sanders (1991)

13 What about our Milky Way Galaxy? We are in a lousy location – inside the disk, far from the center – Can’t see (at optical wavelengths) very far along directions in the disk (~ 1 kpc). – The Sun is highly likely to be participating in the local circular orbits of stars about the Galactic Center Moving reference frame (Ugh) – Maybe measure ‘Differential Rotation’ locally? “Flat Rotation Curve” + increasing radii = differential rotation Speed the same, distance isn’t

14 Jan Oort and his constants

15 Galactic Longitude L Radial Velocity Of Nearby stars Radial Velocity of distant stars Tangential Velocity of distant stars 000>0 900<00 18000<0 2700>00 36000>0

16 In equation form…

17 http://upload.wikimedia. org/wikipedia/commons /0/0b/Oortmeasure.jpg

18

19 Enter Radio Astronomy Radio wavelengths don’t suffer the extinction seen at optical and near-infrared wavelengths Can ‘see’ through the entire Galactic disk Great! No, wait… I don’t see stars… ‘Clouds’ of gas (‘atomic’ if H I, ‘molecular’ if H 2 – or its tracer CO) Complex emission spectral lines along each line of sight that goes through multiple clouds

20 Stack up spectra versus Longitude

21 Find the “Tangent Points” vs L http://ay201b.files.wordpress.com/2011/03/galactic- kinematics.jpg Then, remap Tangent Velocities with L projection of  0 to reveal circular velocity dependence on R OK, but also trying to find Milky Way spiral arms – they are associated with star formation, which HI isn’t Survey in CO and repeat tangent analysis UMASS-Stony Brook CO survey of the 1980s

22 CO traces H 2, which traces Star Formation Potential Dame, Hartmann, & Thaddeus (2001) ApJ, 547, 792

23 Run of RV with L http://inspirehep.net/record/789176/files/f1_dame.png

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25 Covert RV vs L to  (R)

26

27 Rotation curve + full CO survey = remap H 2 distribution as ‘face-on’ view

28 Criticisms Dips unphysical – too fast for Keplerian R 0,  0 now different than assumed (Reid+) Circular rotation assumption likely not fully correct – Spiral arms have kinematic perturbations Tangent analysis doesn’t work in outer galaxy – Had to adopt other, weaker, methods Others have updated with modern data 13 CO less optically-thick than 12 CO – Better at isolating clouds and arms – Galactic Ring Survey (Jackson+06)

29 HII Region Discovery Survey (Bania+)

30 HII Regions trace spiral arms best http://cdn4.sci- news.com/images/enlarge/image_1649e- Milky-Way-Arms.jpg

31 Galactic Rotation: Back to the Stars APOGEE – multi- fiber high-resolution near-infrared spectroscopy of stars in the Milky Way – Spectral types, luminosity classes, RVs GAIA – direct parallaxes, RVs for up to 1 billion stars in the Milky Way

32 Analysis = Bayesian (a story for another day…) 2012

33 Mass Models, Dark Matter, Galaxy Assemblage http://milkyway.cs.rpi.edu/download/ima ges/gal_rotation_curve.png http://www.stsci.edu/~inr/t hisweek1/thisweek/cloudstr eam.jpg


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