the warm-hot gaseous halo of the milky way

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The Warm-hot Gaseous Halo of the Milky Way Smita Mathur The Ohio State University With Anjali Gupta, Yair Krongold, Fabrizio Nicastro, M.

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The Warm-hot Gaseous Halo of the Milky Way. Smita Mathur The Ohio State University With Anjali Gupta, Yair Krongold, Fabrizio Nicastro, M. Galeazzi. In the low-redshift Universe, baryons are missing on all scales. Galaxies. Universe. Clusters. Where are the Galactic missing baryons?. - PowerPoint PPT Presentation

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Page 1: The Warm-hot Gaseous Halo of the Milky Way

The Warm-hot Gaseous Halo of the Milky Way

Smita MathurThe Ohio State University

WithAnjali Gupta, Yair Krongold,

Fabrizio Nicastro, M. Galeazzi

Page 2: The Warm-hot Gaseous Halo of the Milky Way

In the low-redshift Universe, baryons are missing on all scales

Galaxies Clusters Universe

Page 3: The Warm-hot Gaseous Halo of the Milky Way

Where are the Galactic missing baryons?

Local WHIM filamentscale length > 1 Mpc

Local Group Medium scale length of ~ 1 Mpc

Circum-Galactic Medium: extending up to the virial radius (~250kpc)

105 K < T < 107 K

Page 4: The Warm-hot Gaseous Halo of the Milky Way

Simulations of the CGM

Stinson et al. 2011

Page 5: The Warm-hot Gaseous Halo of the Milky Way

Diffuse Warm-hot CGM

Page 6: The Warm-hot Gaseous Halo of the Milky Way

z = 0 z = 0 X-ray Absorption

In several high S/N Chandra In several high S/N Chandra and XMM spectraand XMM spectra

• OVII absorption (@21.60 Å)OVII absorption (@21.60 Å)

• Sometimes OVIII (@18.96 Å)Sometimes OVIII (@18.96 Å) and/or Ne IX (@13.44 Å)and/or Ne IX (@13.44 Å)

Mathur et al. 2003

Page 7: The Warm-hot Gaseous Halo of the Milky Way

Z=0 X-ray absorption

Page 8: The Warm-hot Gaseous Halo of the Milky Way

PKS 2155-304 PKS 2155-304 Nicastro et al. 2002Nicastro et al. 2002

Page 9: The Warm-hot Gaseous Halo of the Milky Way

z = 0 X-ray Absorption• In several high S/N Chandra spectra:

– Mkn 421 (Williams et al. 2005) – Mkn 279 (Williams et al. 2006) – PKS 2155-304 (Nicastro et al. 2002)– 3C 273 (Fang et al. 2003)– Other sightlines with lower significance

(McKernan et al 2004)

• Always OVII, sometimes other species• Chandra-LETG resolution 700 km/s, so all

lines are unresolved

Page 10: The Warm-hot Gaseous Halo of the Milky Way

Origin

• Hot Galactic Halo/Corona…– From galaxy formation / feedback processes– Some OVII seen within 50 kpc (Wang et al.

2005)

• … or Local Warm-Hot IGM?– Predicted by simulations (Kravtsov et al. 2002)– Upper limit on OVII emission implies very low

density (Rasmussen et al. 2003)

Page 11: The Warm-hot Gaseous Halo of the Milky Way

Our Chandra Survey of Our Chandra Survey of OOVIIVII and O and OVIIIVIII

Chandra sight lines Previous OVII detection

Page 12: The Warm-hot Gaseous Halo of the Milky Way

Our Chandra Survey of Our Chandra Survey of OVII and OVIIIOVII and OVIII

• 29 sight lines with good S/N near OVII z=0 29 sight lines with good S/N near OVII z=0 regionregion• OOVIIVII detection in 21 sight lines detection in 21 sight lines• OOVIIIVIII detection in 8 sight lines detection in 8 sight lines

Page 13: The Warm-hot Gaseous Halo of the Milky Way

OVII EW DistributionOVII EW Distribution ___ OVII detection ----- OVII upper limit

Page 14: The Warm-hot Gaseous Halo of the Milky Way

OVII OVIII

OVII and OVIII z=0 AbsorptionOVII and OVIII z=0 Absorption

• Log T = 6.1-6.4 KLog T = 6.1-6.4 K

Page 15: The Warm-hot Gaseous Halo of the Milky Way

Column Density Measurement• Optically thin line

N(ion) = 1.3 × 1020 (EW/f λ2) cm-2

• For OVII EW(Kβ)/EW(Kα) = 0.156

Most of OVII KMost of OVII Kαα are saturated are saturated

Page 16: The Warm-hot Gaseous Halo of the Milky Way

log(Nlog(NOVIIOVII) and b contour) and b contour

Page 17: The Warm-hot Gaseous Halo of the Milky Way

• Log NLog NOVIIOVII = 16.19 ± 0.08 cm = 16.19 ± 0.08 cm-2-2

2-3 times higher than previous estimates2-3 times higher than previous estimates

• Column density NColumn density NHH==μμ n neeL L

Page 18: The Warm-hot Gaseous Halo of the Milky Way

Galactic Halo Emission MeasureGalactic Halo Emission Measure

Henley et al. (2010) using XMM-Newton

Yoshino et al. (2009) using Suzaku• Galactic Halo temperature is fairly constant

T = (1.8 -2.4) × 106 K

• Halo emission measure varies by an order of magnitude

EM = (0.0005 – 0.005) cm-6 pc

EM = 0.003 (Z/ZΘ) cm-6 pc

Page 19: The Warm-hot Gaseous Halo of the Milky Way

Combining Absorption and Emission Measurement Breaks the degenaracy

nnee = (2.0 ± 0.6 )× 10 = (2.0 ± 0.6 )× 10−4−4(0.5/f(0.5/fOVIIOVII))−1−1 cm cm−3−3

R = (71.8 ± 30.2) x

(8.51 × 104/(AO/AH))(0.5/f(0.5/fOVIIOVII))22(Z(ZΘΘ/Z) kpc/Z) kpc

Page 20: The Warm-hot Gaseous Halo of the Milky Way

Mass Probed by OVII and OVIII X-ray Absorbing/Emitting Gas Phase

M M totaltotal > 1.7 × 10 > 1.7 × 1099 (fc/0.72) (8.51 × 10-4/(AO/AH))3(0.5/fOVII)5(ZΘ/Z)3MMΘΘ

For Z = 0.3ZFor Z = 0.3ZΘΘ

L > 138 kpcL > 138 kpc

MMtotaltotal > 6.1 × 10 > 6.1 × 101010 M MΘΘ

Gupta, Mathur + 2012, 2014

Page 21: The Warm-hot Gaseous Halo of the Milky Way

Courtesy: Chandra presss office

Page 22: The Warm-hot Gaseous Halo of the Milky Way

Fang, Bullock +2012

Page 23: The Warm-hot Gaseous Halo of the Milky Way

This is a robust result!

• Is the z=0 absorption mostly from the Galactic disk? No.

• What about the uniform density profile? No problem: gives a lower limit on mass.

• Are the emission and absorption at different temperatures? No.

Page 24: The Warm-hot Gaseous Halo of the Milky Way

….. no anticorrelation with Galactic latitude

In emission In absorption

Henley et al 2013 (XMM) Gupta et al. 2014

Page 25: The Warm-hot Gaseous Halo of the Milky Way

Future directions• Probing the anisotropy: emission and

absorption along the same sightline.

-- New Suzaku observations

-- New XMM-Newton Observations.

• Different density and temperature profiles: e.g. Maller-Bullock profile in NFW halo.

• Probing the multi-phase medium: other ions dominant at different temperatures.

Page 26: The Warm-hot Gaseous Halo of the Milky Way

ConclusionConclusion• X-rays provides evidence for hot (T>106 K) gas in and around the Milky Way.

• X-ray OVII and O VIII absorption lines at z=0 probe the hot gas extending over a large region around the Milky Way, with a radius of over 100 kpc.

•The mass content of this phase is over 1010 MΘ.

•A large fraction of Galactic missing baryons are in this hot phase.

•Appears to be a robust result supported by theoretical models.