Probing the electron-to-proton mass ratio gradient in the Milky Way with Class I methanol masers

Author:

Levshakov S A123,Agafonova I I3,Henkel C456,Kim Kee-Tae78,Kozlov M G23,Lankhaar B9,Yang W4

Affiliation:

1. Ioffe Physical-Technical Institute, Saint Petersburg, 194021, Russia

2. Petersburg Nuclear Physics Institute of NRC ‘Kurchatov Institute’, Gatchina, Leningrad District, 188300, Russia

3. Department of Physics, Electrotechnical University ‘LETI’, Saint Petersburg, 197376, Russia

4. Max Planck Institut für Radioastronomie, Auf dem Hügel 69, Bonn 53121, Germany

5. Department of Astronomy and Space Science, King Abdulaziz University, PO Box 80203, Jeddah 21589, Saudi Arabia

6. Xinjiang Astronomical Observatory, Chinese Academy of Sciences, Urumqi 830011, People’s Republic of China

7. Korea Astronomy and Space Science Institute, 776 Daedeokdae-ro, Yuseong-gu, Daejeon 34055, Republic of Korea

8. University of Science and Technology, Korea (UST), 217 Gajeong-ro, Yuseong-gu, Daejeon 34113, Republic of Korea

9. Department of Space, Earth and Environment, Onsala Space Observatory, Chalmers University of Technology, Onsala, 43992, Sweden

Abstract

ABSTRACT We estimate limits on non-universal coupling of hypothetical hidden fields to standard matter by evaluating the fractional changes in the electron-to-proton mass ratio, μ = me/mp, based on observations of Class I methanol masers distributed in the Milky Way disc over the range of the Galactocentric distances $4 \lesssim R \lesssim 12$ kpc. The velocity offsets ΔV = V44 − V95 measured between the 44- and 95-GHz methanol lines provide, so far, one of the most stringent constraints on the spatial gradient kμ ≡ d(Δμ/μ)/dR < 2 × 10−9 kpc−1 and the upper limit on Δμ/μ <2 × 10−8, where Δμ/μ = $(\mu _{\rm \scriptscriptstyle obs}-\mu _{\rm \scriptscriptstyle lab})/\mu _{\rm \scriptscriptstyle lab}$. We also find that the offsets ΔV are clustered into two groups which are separated by $\delta _{\scriptscriptstyle \Delta V} = 0.022 \pm 0.003$ km s−1 (1σ confidence level). The grouping is most probably due to the dominance of different hyperfine transitions in the 44- and 95-GHz methanol maser emission. Which transition becomes favoured is determined by an alignment (polarization) of the nuclear spins of the four hydrogen atoms in the methanol molecule. This result confirms that there are preferred hyperfine transitions involved in the methanol maser action.

Funder

Russian Science Foundation

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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