Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui...

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Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui Nagoya University Southern Observatories CTA meeting April 16-17, 2015, Adelaide 1

Transcript of Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui...

Page 1: Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui Nagoya University Southern Observatories CTA meeting April.

Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays 

Yasuo FukuiNagoya UniversitySouthern Observatories  

CTA meeting

April 16-17, 2015, Adelaide

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Page 2: Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui Nagoya University Southern Observatories CTA meeting April.

ISM

Interstellar medium ISM between stars

ISM consists of gas and dust Mgas/Mdust is 100, dust grains include most of the heavy elements; H:He:CNO = 1:10-1:10-4

Gas consists of neutral and ionized components Neutral is dominant, related to star formation

Neutral consists of molecular and atomic gas 1951 discovery of 21cm HI 1970 discovery of 2.6mm CO [H2 has no suitable transition]

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HI is assumed to be optically thin in text books

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Molecular vs. atomic

HI gas: average density 1 cm-3, Tk=125K “assumption, 21cm line optically thin”--NHI=1.8e18 WHI

Dark gas: gamma rays (pp reaction p0 2g), dust extinction “cannot be seen in HI or CO”--CO-free H2?

H2 gas: density 1000 cm-3, Tk=10K “CO 2.6mm line via Xco factor”--NH2=Xco Wco (factor of 2 uncertainty)

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Kalberla+ 2005Courtesy of Legacy Archive for Microwave Background Data Analysis

The Leiden/Argentine/Bonn Galactic HI Survey

HI LAB

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GeV Gamma rays

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Planck Collaboration, arXiv:1101.2029

CO surveys : CfA + NANTEN

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Isabelle Grenier et al. Science 2005

Column density of dark gas ~ 1020.5-1021.5 /cm2

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Nearby cloud without background source [Fukui+ 2014]

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MBM 53, 54, 55tau353-WHI 相関プロット

HI dust correlation is bad

Planck sub-mm data

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Page 11: Accurate measurement of interstellar hydrogen as the target of hadronic gamma rays Yasuo Fukui Nagoya University Southern Observatories CTA meeting April.

MBM 53, 54, 55tau353-WHI 相関プロット

HI dust correlation is bad

Planck sub-mm data

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Td highestHI is thin

With Td decreaseHI becomes thick

Fukui+ 2014; 2015

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Fig. 3

Ts=10, 20, 30, …, 100 K

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All sky Planck tau353: Fukui+2015

masked in gray [double HI profiles/Ha/CO/Plane]

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Excess NHI=“Dark gas”

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Planck Collaboration, arXiv:1101.2029

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Planck Collaboration, arXiv:1101.2029

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HI becomes dark at higher density

Goldsmith et al. 200720

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Step 1We estimate the W(HI) range

Step 2Estimating a conversion factorform W(HI) to NH using linierfitting

Step 3We apply the correction

Tau 353 vs. W(HI)

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(left) Image: Total interstellar proton column density, contours: TeV γ-rays (Aharonian+07)(Right) Azimuthal plots

Fukui, Sano+15 in prep.

Vela Jr. total ISM protons & TeV γ-rays

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Vela Jr. total ISM protons & TeV γ-rays(optically thick HI corrected)

(left) Image: Total interstellar proton column density, contours: TeV γ-rays (Aharonian+07)(Right) Azimuthal plots

Fukui, Sano+15 in prep.

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RX J1713.7-3946: Interstellar proton vs. TeV gamma rays

Fukui et al. 2012HI + 2H2

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Dark HI SE Cloud (Self-Absorption)

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HI self absorption

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Very accurate measurement of both atomic/molecular hydrogen has become possible by “truly optically thin HI”

HI gas: average density 1 cm-3, Tk=125K “assumption, 21cm line optically thin”--NHI=1.8e18 x WHI but HI is optically thick

Dark gas: gamma rays (pp reaction p0 2g), dust extinction. CTA will play a major role

H2 gas: density 1000 cm-3, Tk=10K “CO 2.6mm line via Xco factor”--NH2=Xco x Wco (factor of 2 uncertainty)

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