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Gauging low-metallicity turbulence in the small Magellanic cloud

Gauging low-metallicity turbulence in the small Magellanic cloud

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<strong>Gaug<strong>in</strong>g</strong> Low-<strong>metallicity</strong><br />

Turbulence <strong>in</strong> <strong>the</strong> Small<br />

Blakesley Burkhart<br />

University of Wiscons<strong>in</strong><br />

Madison<br />

Alex Lazarian (UW)<br />

S. Stanimirovic (UW); G. Kowal (Univ. Sao<br />

Paulo); J. Cho (Chungnam National Univ.)<br />

Freitag, 19. Oktober 12


Magnetic fields & <strong>turbulence</strong><br />

are critically important for<br />

many astrophysical<br />

processes <strong>in</strong> <strong>low</strong> and high<br />

<strong>metallicity</strong> regions....<br />

…and connect a<br />

wide<br />

range of scales!<br />

Sub AU AU Pc Kpc Mpc<br />

Freitag, 19. Oktober 12


The story of this talk: How to Study<br />

Turbulence From <strong>the</strong> Observations<br />

Tool box for study<strong>in</strong>g<br />

MHD <strong>turbulence</strong>:<br />

Statistical<br />

Studies/<br />

Scal<strong>in</strong>g Laws<br />

=<br />

=<br />

Theory<br />

Insight <strong>in</strong>to <strong>the</strong> Physics<br />

of <strong>the</strong> Observations<br />

Numerics<br />

Theory predicts and<br />

generalizes<br />

=<br />

Numerics al<strong>low</strong>s <strong>low</strong><br />

resolution test<strong>in</strong>g<br />

Freitag, 19. Oktober 12


Q. What Information do we need to study<br />

<strong>turbulence</strong><br />

Ultimately….we need <strong>the</strong> cascade!<br />

E(k)~-5/3k<br />

Or -11/3K for 3D<br />

Inertial range slope gives <strong>the</strong> cascad<strong>in</strong>g rate and depends on <strong>the</strong> compressibility<br />

and (to a lesser<br />

extent) <strong>the</strong> magnetization.<br />

Question: How to obta<strong>in</strong> sonic Mach number, power spectrum, and<br />

magnetization <strong>in</strong> ISM observations<br />

Freitag, 19. Oktober 12


Q. How to Obta<strong>in</strong> Information on MHD<br />

Turbulence<br />

Ultimately….we need <strong>the</strong> casca<br />

E(k)~-5/3k<br />

Freitag, 19. Oktober 12


Observational Tests Case: The SMC<br />

SMC is <strong>the</strong> ideal observational<br />

candidate for a study of <strong>low</strong><br />

<strong>metallicity</strong> <strong>turbulence</strong> :<br />

Freitag, 19. Oktober 12<br />

1)At 60kpc away it is close and<br />

we ignore distance confusion<br />

that exists <strong>in</strong> MW.<br />

2) Heavy element abundance is<br />

~10 <strong>low</strong>er <strong>the</strong>n MW.<br />

3) Well studied dwarf galaxy <strong>in</strong><br />

many wavelengths of<br />

emission/absorption with<br />

magnetic field <strong>in</strong>formation….


Outl<strong>in</strong>e<br />

•The SMC <strong>in</strong> 21 cm emission<br />

•Obta<strong>in</strong><strong>in</strong>g Velocity and Density Spectrum <strong>in</strong> <strong>the</strong> SMC via HI<br />

radio data and comparison with simulations<br />

•Obta<strong>in</strong><strong>in</strong>g <strong>the</strong> compressibility (sonic Mach number) of <strong>the</strong><br />

SMC via sp<strong>in</strong>/k<strong>in</strong>etic temperatures and Probability<br />

Distribution Function moments and comparison with<br />

simulations<br />

•Issues of large scale driv<strong>in</strong>g as traced by PDFs<br />

Freitag, 19. Oktober 12


SMC <strong>in</strong> 21 cm emission<br />

Radio data is ideal for studies of <strong>turbulence</strong> because it<br />

conta<strong>in</strong>s <strong>in</strong>formation about <strong>turbulence</strong> velocity along <strong>the</strong><br />

LOS<br />

Stanimirovic et al. 1999 data set has good spatial (98”)<br />

and spectral resolution (1.65kms -1 ) and conta<strong>in</strong>s both<br />

s<strong>in</strong>gle dish (Parkes Telescope) and <strong>in</strong>terferometer (ATCA<br />

telescope) data (30pc-4kpc).<br />

Freitag, 19. Oktober 12


Determ<strong>in</strong><strong>in</strong>g <strong>the</strong> Velocity/Density Spectrum of Turbulence <strong>in</strong> t<br />

SMC<br />

Turbulence broadens emission and absorption l<strong>in</strong>es and this can be used<br />

to study <strong>turbulence</strong> with VCA techniques<br />

Freitag, 19. Oktober 12<br />

Developed <strong>in</strong> Lazarian & Pogosyan<br />

00, 04


Determ<strong>in</strong><strong>in</strong>g <strong>the</strong> Velocity/Density Spectrum of Turbulence <strong>in</strong> t<br />

SMC<br />

Turbulence broadens emission and absorption l<strong>in</strong>es and this can be used<br />

to study <strong>turbulence</strong> with VCA techniques<br />

Freitag, 19. Oktober 12<br />

Developed <strong>in</strong> Lazarian & Pogosyan<br />

00, 04


Determ<strong>in</strong><strong>in</strong>g <strong>the</strong> Velocity/Density Spectrum of Turbulence <strong>in</strong> t<br />

SMC<br />

Turbulence broadens emission and absorption l<strong>in</strong>es and this can be used<br />

to study <strong>turbulence</strong> with VCA techniques<br />

Freitag, 19. Oktober 12<br />

Developed <strong>in</strong> Lazarian & Pogosyan<br />

00, 04


Determ<strong>in</strong><strong>in</strong>g <strong>the</strong> Velocity/Density Spectrum of Turbulence <strong>in</strong> t<br />

SMC<br />

Turbulence broadens emission and absorption l<strong>in</strong>es and this can be used<br />

to study <strong>turbulence</strong> with VCA techniques<br />

Freitag, 19. Oktober 12<br />

Developed <strong>in</strong> Lazarian & Pogosyan<br />

00, 04


Determ<strong>in</strong><strong>in</strong>g <strong>the</strong> Velocity/Density Spectrum of Turbulence <strong>in</strong> t<br />

SMC<br />

Turbulence broadens emission and absorption l<strong>in</strong>es and this can be used<br />

to study <strong>turbulence</strong> with VCA techniques<br />

VCA<br />

procedure<br />

Freitag, 19. Oktober 12<br />

Developed <strong>in</strong> Lazarian & Pogosyan<br />

00, 04


Density<br />

Spectral slope -3.3<br />

Indicates superson<br />

motions.<br />

Velocity/Density Power Spectrum<br />

<strong>in</strong> <strong>the</strong> SMC<br />

Application of VCA to SMC from Stanimirovic & Lazarian 2001<br />

Q: Power law<br />

seen<br />

For all scales….<br />

What drives<br />

Turbulence <strong>in</strong> <strong>the</strong><br />

SMC<br />

Freitag, 19. Oktober 12


Density Spectrum Compared with<br />

3D MHD Simulations<br />

Density spectral <strong>in</strong>dex=-3.3 for SMC<br />

From Burkhart et al.<br />

2010<br />

Low B<br />

High B<br />

Freitag, 19. Oktober 12


Sonic Mach Number<br />

• Heiles and Troland (2003) showed that <strong>the</strong> Mach number can be related to<br />

<strong>the</strong> ratio of upper limit of <strong>the</strong> k<strong>in</strong>etic temperature (T k ) and <strong>the</strong> sp<strong>in</strong><br />

temperature (T s ).<br />

• Us<strong>in</strong>g absorption sources from 29 strong radio cont<strong>in</strong>uum sources (Dickey<br />

et al. 2000) we derive T k = (FWHM/0.215) 2 and use Dickey et al. (2000)<br />

values for T s . Trac<strong>in</strong>g CNM<br />

Freitag, 19. Oktober 12<br />

M s


Sonic Mach Number from PDFs<br />

Long time tool of studies of <strong>turbulence</strong> of column density data for WNM/CNM<br />

and Molecular Clouds<br />

2 nd moment: Variance (σ 2 l<strong>in</strong>ear and log PDF) vs. M s<br />

3 rd moment: Skewness(l<strong>in</strong>ear PDF) vs. MS=A*M s s +b<br />

K=A*M s +b See papers by: Kowal,<br />

Burkhart, Federrath, Col<strong>in</strong>s,<br />

Padoan, Vazquez-Semadeni,<br />

Mol<strong>in</strong>a…<br />

L<strong>in</strong>ear Column Density PDF<br />

4 th moment: Kurtosis(l<strong>in</strong>ear PDF) vs. M s<br />

Ms=0.5<br />

M s =0.5<br />

Freitag, 19. Oktober 12


Sonic Mach Number from PDFs<br />

Long time tool of studies of <strong>turbulence</strong> of column density data for WNM/CNM<br />

and Molecular Clouds<br />

2 nd moment: Variance (σ 2 l<strong>in</strong>ear and log PDF) vs. M s<br />

3 rd moment: Skewness(l<strong>in</strong>ear PDF) vs. MS=A*M s s +b<br />

K=A*M s +b See papers by: Kowal,<br />

Burkhart, Federrath, Col<strong>in</strong>s,<br />

Padoan, Vazquez-Semadeni,<br />

Mol<strong>in</strong>a…<br />

L<strong>in</strong>ear Column Density PDF<br />

4 th moment: Kurtosis(l<strong>in</strong>ear PDF) vs. M s<br />

Ms=0.5 Ms=2.0<br />

M s =2.0<br />

Freitag, 19. Oktober 12


Sonic Mach Number from PDFs<br />

Long time tool of studies of <strong>turbulence</strong> of column density data for WNM/CNM<br />

and Molecular Clouds<br />

2 nd moment: Variance (σ 2 l<strong>in</strong>ear and log PDF) vs. M s<br />

3 rd moment: Skewness(l<strong>in</strong>ear PDF) vs. MS=A*M s s +b<br />

K=A*M s +b See papers by: Kowal,<br />

Burkhart, Federrath, Col<strong>in</strong>s,<br />

Padoan, Vazquez-Semadeni,<br />

Mol<strong>in</strong>a…<br />

L<strong>in</strong>ear Column Density PDF<br />

4 th moment: Kurtosis(l<strong>in</strong>ear PDF) vs. M s<br />

Ms=0.5 Ms=2.0 Ms=4.5<br />

M s =4.5<br />

Freitag, 19. Oktober 12


Sonic Mach Number from PDFs<br />

Long time tool of studies of <strong>turbulence</strong> of column density data for WNM/CNM<br />

and Molecular Clouds<br />

2 nd moment: Variance (σ 2 l<strong>in</strong>ear and log PDF) vs. M s<br />

3 rd moment: Skewness(l<strong>in</strong>ear PDF) vs. MS=A*M s s +b<br />

K=A*M s +b See papers by: Kowal,<br />

Burkhart, Federrath, Col<strong>in</strong>s,<br />

Padoan, Vazquez-Semadeni,<br />

Mol<strong>in</strong>a…<br />

L<strong>in</strong>ear Column Density PDF<br />

4 th moment: Kurtosis(l<strong>in</strong>ear PDF) vs. M s<br />

Ms=0.5 Ms=2.0 Ms=4.5 Ms=8.0<br />

M s =8.0<br />

Freitag, 19. Oktober 12


Sonic Mach Number: PDF vs.<br />

skewness<br />

kurtosis<br />

M s<br />

M s<br />

Observational Method for Cold Neutral SMC<br />

Mach Numbers<br />

Freitag, 19. Oktober 12<br />

M s


GASKAP (PI: Dickey): MW plane +<br />

<strong>Magellanic</strong> System<br />

5000+ HI absorption spectra build 2d<br />

images of CNM temperature and fraction<br />

HI+OH emission turbulent properties and<br />

atomic/molecular transition<br />

GAMES with WSRT<br />

(nor<strong>the</strong>rn sister survey, PI:<br />

McClure-Griffiths):<br />

HI absorption + HI/OH emission<br />

Toge<strong>the</strong>r, measure how CNM properties<br />

vary with <strong>in</strong>terstellar environments<br />

(MW, LMC, SMC).<br />

ASKAP<br />

Freitag, 19. Oktober 12<br />

Dickey et al. (2012)<br />

https://sites.google.com/site/<br />

gaskapproject/<br />

Westerbork &<br />

Apertif


Q. What is <strong>the</strong> driv<strong>in</strong>g scale<br />

Skewness<br />

“Moment<br />

Maps”<br />

Kurtosis<br />

Several regions <strong>in</strong> <strong>the</strong> SMC <strong>in</strong>dicate very quiescent environments, most of <strong>the</strong>m<br />

unfortunately have a size close to our angular resolution (30’ after <strong>the</strong> kernal is<br />

applied).<br />

Regions with <strong>the</strong> highest sonic Mach number via PDF analysis are found around<br />

<strong>the</strong> bar and correspond to compressed HI contours.<br />

Most high M s regions seem to trace shear f<strong>low</strong>s. Several are near LMC<br />

Freitag, 19. Oktober 12


Summary<br />

1) HI gas <strong>in</strong> <strong>the</strong> SMC density/velocity<br />

spectrum corresponds to mildly<br />

supersonic <strong>turbulence</strong><br />

2) Spectrum shows no evidence of a<br />

turn over!<br />

3) Sp<strong>in</strong>-K<strong>in</strong>etic temperatures show <strong>the</strong><br />

SMC to be generally supersonic which<br />

agrees with PDF analysis predicted by<br />

MHD simulations<br />

4) Evidence for large scale external<br />

driv<strong>in</strong>g <strong>in</strong> SMC<br />

PDFs - Burkhart et al., 09, ApJ, 693, 250;<br />

Kowal et al. 07, ApJ, 658, 423<br />

Velocity Power Spectrum (VCS/VCA)- Lazarian & Pogosyan,08, ApJ,<br />

686, 350;<br />

Stanimirovic & Lazarian, 2001, ApJ, 551,<br />

53<br />

Chepurnov, Burkhart & Lazarian, <strong>in</strong><br />

prep.<br />

Freitag, 19. Oktober 12


What about <strong>the</strong> magnetic<br />

fields!<br />

Freitag, 19. Oktober 12


Summary<br />

1) HI gas <strong>in</strong> <strong>the</strong> SMC density/velocity<br />

spectrum corresponds to mildly<br />

supersonic <strong>turbulence</strong><br />

2) Spectrum shows no evidence of a<br />

turn over!<br />

3) Sp<strong>in</strong>-K<strong>in</strong>etic temperatures show <strong>the</strong><br />

SMC to be generally supersonic which<br />

agrees with PDF analysis predicted by<br />

MHD simulations<br />

4) Evidence for large scale external<br />

driv<strong>in</strong>g <strong>in</strong> SMC<br />

PDFs - Burkhart et al., 09, ApJ, 693, 250;<br />

Kowal et al. 07, ApJ, 658, 423<br />

Velocity Power Spectrum (VCS/VCA)- Lazarian & Pogosyan,08, ApJ,<br />

686, 350;<br />

Stanimirovic & Lazarian, 2001, ApJ, 551,<br />

53<br />

Chepurnov, Burkhart & Lazarian, <strong>in</strong><br />

prep.<br />

Freitag, 19. Oktober 12


Freitag, 19. Oktober 12<br />

Thermal <strong>in</strong>stability…

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