1
Non-solar chemical composition in the multiphase hot halo of Milky Way Sanskriti Das 1 ([email protected]), Smita Mathur 1,2 (1)Department of Astronomy, (2)Center for Cosmology & Astroparticle Physics, The Ohio State University Introduction The halo of Milky Way is known to be hot, extended, massive and anisotropic [1, 2, 3]. The halo is pictured as an isothermal sphere at T = 10 6.3 K, the virial tem- perature (fig. 1), and is assumed to have solar chem- ical composition. Shallow observations are unable to probe any finer thermal and chemical information. Figure 1:Hot gaseous halo of Milky Way [1] (https: //www.nasa.gov/mission_pages/chandra/multimedia/ hot_gas_halo.html) Objective Characterize the hot (> 10 6 K) halo of Milky Way using Ms long imaging spectra in emission and grating spectra in absorption Summary There are 3–4 discrete phases at 10 5.8 K <T 6 10 7.4 K coexisting in the halo of Milky Way [5]. The abundance ratios in the hot halo of Milky Way are non-solar. This gives important insights into the chemical evolution of the Galaxy [4]. The mass of the multiple temperature components and the non-solar chemical composition have great implications for missing baryons and missing metals. Future directions Our Chandra archival proposal to extend this study along many sightlines has been accepted Acknowledgements We thank our collaborators, Anjali Gupta, Yair Krongold, and Fabrizio Nicastro. The grants from NASA and the data from ESA are gratefully acknowledged. References [1] Gupta, A., Mathur, S. et al., 2012, APJL, 756, 8 [2] Gupta, A., Mathur, S. et al., 2014, Ap&SS, 352, 775 [3] Gupta, A., Mathur, S. & Krongold, Y., 2017, ApJ, 836, 243 [4] Das, S., Mathur, S. et al. 2019, ApJL, 882, L23 [5] Das, S., Mathur, S. et al. 2019, ApJ, in press Result-I: The hot halo of Milky Way is NOT a single phase [5] We analyze deep (t exp = 1.85 Ms) XMM-Newton spectra toward and around the blazar 1ES 1553+113 probing the hot Milky Way halo in absorption and emission with unprecedented sensitivity. Figure 2:The unfolded spectra of 1ES 1553+113 with the absorption features from the Milky Way halo, and the best-fit model with two halo components: T=10 6.07-6.13 K and T=10 6.96-7.15 K. Figure 3:The emission spectra around the sightline toward 1ES 1553+113, and the best-fit model with two halo compo- nents: T=10 6.25-6.42 K and T=10 6.68-6.92 K. Figure 4:Multiple temperature components in the hot halo of Milky Way [5] Result-II: The abundance ratios in the hot halo are NOT solar [4] Figure 5:The absorption lines of the detected neon and nitrogen lines for the best-fit non-solar (yellow lines) vs. solar (blue lines) abundance ratios relative to oxygen. [Ne/O] and [N/O] are super-solar, and [Ne/N] is solar: [Ne/O]=[N/O]=0.7 +1.6 -0.2 (>99.73% confidence). This implies a) Type-II Supernovae en- richment, b) AGB stars enrichment, c) oxygen’s efficient cooling and depletion onto dust. Figure 6:The absorption profile for the solar [Ne/Fe] (yellow lines) vs. the best-fit non-solar [Ne/Fe] (blue lines). The vertical black line at 12.13 Å corresponds to Ne x Ly-α line. [Ne/Fe] is super-solar: [Ne/Fe] = 1.6 +1.2 -0.4 (>99.73% confidence). [O/Fe] =0.9 +0.7 -0.3 (>99.73% confidence) is super-solar too. This indicates α- enhancement, and possible depletion of iron onto inter- stellar and/or circumgalactic dust.

Non-solar chemical composition in the multiphase hot halo ... · Non-solar chemical composition in the multiphase hot haloof Milky Way Sanskriti Das1 ([email protected]),

  • Upload
    others

  • View
    1

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Non-solar chemical composition in the multiphase hot halo ... · Non-solar chemical composition in the multiphase hot haloof Milky Way Sanskriti Das1 (das.244@buckeyemail.osu.edu),

Non-solar chemical composition in themultiphase hot halo of Milky Way

Sanskriti Das1 ([email protected]), Smita Mathur1,2

(1)Department of Astronomy, (2)Center for Cosmology & Astroparticle Physics, The Ohio State University

Introduction

The halo of Milky Way is known to be hot, extended,massive and anisotropic [1, 2, 3]. The halo is picturedas an isothermal sphere at T = 106.3 K, the virial tem-perature (fig. 1), and is assumed to have solar chem-ical composition. Shallow observations are unable toprobe any finer thermal and chemical information.

Figure 1:Hot gaseous halo of Milky Way [1] (https://www.nasa.gov/mission_pages/chandra/multimedia/hot_gas_halo.html)

Objective

Characterize the hot (> 106 K) halo of MilkyWay using Ms longimaging spectra in emission and grating spectra in absorption

Summary

•There are 3–4 discrete phases at 105.8K< T 6 107.4K coexisting in the halo ofMilky Way [5].

•The abundance ratios in the hot haloof Milky Way are non-solar. This givesimportant insights into the chemicalevolution of the Galaxy [4].

•The mass of the multiple temperaturecomponents and the non-solarchemical composition have greatimplications for missing baryons andmissing metals.

Future directions

Our Chandra archival proposal to extend this study alongmany sightlines has been accepted

AcknowledgementsWe thank our collaborators, Anjali Gupta, Yair Krongold, and Fabrizio Nicastro. The grants from NASAand the data from ESA are gratefully acknowledged.

References

[1] Gupta, A., Mathur, S. et al., 2012, APJL, 756, 8[2] Gupta, A., Mathur, S. et al., 2014, Ap&SS, 352, 775[3] Gupta, A., Mathur, S. & Krongold, Y., 2017, ApJ, 836, 243[4]Das, S., Mathur, S. et al. 2019, ApJL, 882, L23[5]Das, S., Mathur, S. et al. 2019, ApJ, in press

Result-I: The hot halo of Milky Way is NOT a single phase [5]

We analyze deep (texp = 1.85 Ms) XMM-Newton spectra toward and around the blazar 1ES 1553+113probing the hot Milky Way halo in absorption and emission with unprecedented sensitivity.

10 15 20 25 30

Wavelength [Å]

10-11

FE [

erg

s cm

−2 s−

1 k

eV−

1] NeX Lyα

NeIX HeαOVII Heβ

OVIII Lyα

OVII Heα

NVII Lyα

NVI HeβNVI Heα

RGS1 RGS2

Figure 2:The unfolded spectra of 1ES 1553+113 with the absorptionfeatures from the Milky Way halo, and the best-fit model with twohalo components: T=106.07−6.13K and T=106.96−7.15K.

0.4 0.5 0.6 0.7 0.8 1.0 1.2

Energy [keV]

10-14

10-13

10-12

10-11

10-10

FE [

erg

s cm

−2 s−

1ke

V−

1]

CV

I Lyβ

OV

II H

OV

III Lyα

+O

VII H

OV

III Lyβ

OV

III Ly

(γ,δ,ε

)

NeIX

Heα

NeX

Lyα

NV

II L

+N

VI H

Total

Foreground

Galactic halo 1

Galactic halo 2

Background

Instrumental

Figure 3:The emission spectra around the sightline toward1ES 1553+113, and the best-fit model with two halo compo-nents: T=106.25−6.42K and T=106.68−6.92K.

5.8 6.0 6.2 6.4 6.6 6.8 7.0 7.2 7.4log (Temperature) [K]

T1 T2 T3 T4

T′3

Absorption:3σ Absorption:1σ Emission

Figure 4:Multiple temperature components in the hot halo of Milky Way [5]

Result-II: The abundance ratios in the hot halo are NOT solar [4]

11.9 12.0 12.1 12.2 12.30.7

0.8

0.9

1.0

1.1

1.2

Norm

aliz

ed F

lux

NeX

13.3 13.4 13.5 13.6 13.70.7

0.8

0.9

1.0

1.1

1.2

NeIX

[Ne/O] ¯

[Ne/O] = ¯

24.5 24.6 24.7 24.8

Wavelength [Å]

0.7

0.8

0.9

1.0

1.1

1.2

Norm

aliz

ed F

lux

NVIIRGS1

RGS2

28.65 28.75 28.85 28.95 29.05

Wavelength [Å]

0.7

0.8

0.9

1.0

1.1

1.2

NVI

[N/O] ¯

[N/O] = ¯

Figure 5:The absorption lines of the detected neon and nitrogenlines for the best-fit non-solar (yellow lines) vs. solar (blue lines)abundance ratios relative to oxygen.

• [Ne/O] and [N/O] are super-solar, and[Ne/N] is solar: [Ne/O]=[N/O]=0.7+1.6

−0.2 (>99.73%confidence). This implies a) Type-II Supernovae en-richment, b) AGB stars enrichment, c) oxygen’s efficientcooling and depletion onto dust.

11.25 11.75 12.25 12.75

Wavelength [Å]

0.7

0.8

0.9

1.0

1.1

Norm

aliz

ed f

lux

NeFe ¯

NeFe = ¯

Figure 6:The absorption profile for the solar [Ne/Fe] (yellow lines)vs. the best-fit non-solar [Ne/Fe] (blue lines). The vertical blackline at 12.13 Å corresponds to Nex Ly-α line.

• [Ne/Fe] is super-solar: [Ne/Fe] = 1.6+1.2−0.4

(>99.73% confidence). [O/Fe] = 0.9+0.7−0.3 (>99.73%

confidence) is super-solar too. This indicates α-enhancement, and possible depletion of iron onto inter-stellar and/or circumgalactic dust.