2024ApJ...976..209Z


Query : 2024ApJ...976..209Z

2024ApJ...976..209Z - Astrophys. J., 976, 209 (2024/December-1)

Slope of Magnetic Field-Density Relation as an Indicator of Magnetic Dominance.

ZHAO M., LI G.-X. and QIU K.

Abstract (from CDS):

The electromagnetic field is a fundamental force in nature that regulates the formation of stars in the Universe. Despite decades of efforts, a reliable assessment of the importance of the magnetic fields in star formation relations remains missing. In star formation research, our acknowledgment of the importance of magnetic fields is best summarized by the R. M. Crutcher et al. B-ρ relation,\begin{eqnarray*}\mathrm{log}B(\rho )/\mathrm{Gauss}=\left\{\begin{array}{l}-5,\,\mathrm{if}\,\rho \,\lesssim \,{10}^{-20}\,{\rm{g}}\,{\mathrm{cm}}^{-3}\\ \displaystyle \frac{2}{3}\cdot \mathrm{log}\rho +\mathrm{log}{\rho }_{0},\,\mathrm{if}\,\rho \,\gtrsim \,{10}^{-20}\,{\rm{g}}\,{\mathrm{cm}}^{-3},\end{array}\right.\end{eqnarray*}whose interpretation remains controversial. The relation is either interpreted as proof of the importance of a magnetic field in gravitational collapse or as the result of self-similar collapse where the role of the magnetic field is secondary to gravity. Using simulations, we find a fundamental relation, ${{ \mathcal M }}_{{\rm{A}}}$-kB–ρ (the slope of the B-ρ relation):\begin{eqnarray*}\displaystyle \frac{{{ \mathcal M }}_{{\rm{A}}}}{{{ \mathcal M }}_{{\rm{A}},{\rm{c}}}}={{\rm{k}}}_{B-\rho }^{{ \mathcal K }}\approx \displaystyle \frac{{{ \mathcal M }}_{{\rm{A}}}}{7.5}\approx {{\rm{k}}}_{B-\rho }^{1.7\pm 0.15}.\end{eqnarray*}This fundamental B-ρ slope relation enables one to measure the Alfvénic Mach number, a direct indicator of the importance of the magnetic field, using the distribution of data in the B-ρ plane. It allows us to apply the following empirical B-ρ relation:\begin{eqnarray*}\displaystyle \frac{B}{{B}_{c}}=\exp \left({\left(\displaystyle \frac{\gamma }{{ \mathcal K }}\right)}^{-1}{\left(\displaystyle \frac{\rho }{{\rho }_{c}}\right)}^{\displaystyle \frac{\gamma }{{ \mathcal K }}}\right)\approx \displaystyle \frac{B}{{10}^{-6.3}{\rm{G}}}\approx \exp \left(9{\left(\displaystyle \frac{\rho }{{10}^{-16.1}{\rm{g}}\,{\mathrm{cm}}^{-3}}\right)}^{0.11}\right)\ ,\end{eqnarray*}which offers an excellent fit to the Crutcher et al. data, where we assume an ${{ \mathcal M }}_{{\rm{A}}}-\rho $ relation ($\tfrac{{{ \mathcal M }}_{{\rm{A}}}}{{{ \mathcal M }}_{{\rm{A}},{\rm{c}}}}={\left(\tfrac{\rho }{{\rho }_{c}}\right)}^{\gamma }\approx {{ \mathcal M }}_{{\rm{A}}}/7.5\approx {\left(\rho /{10}^{-16.1}\,{\rm{g}}\,{{\rm{cm}}}^{-3}\right)}^{0.19}$). The foundational ${{ \mathcal M }}_{{\rm{A}}}-{{\rm{k}}}_{B-\rho }$ relation provides an independent way to measure the importance of the magnetic field against the kinematic motion using multiple magnetic-field measurements. Our approach offers a new interpretation of the classical B-ρ relation, where a gradual decrease in the importance of B at higher densities is implied.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Star formation - Interstellar medium - Interstellar magnetic fields

Simbad objects: 8

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Number of rows : 8
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
2 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1872 0
3 3C 132 rG 04 56 42.922 +22 49 23.06   18.5       ~ 157 1
4 ICRF J050258.4+251625 Sy2 05 02 58.47476282 +25 16 25.2757175   20       ~ 187 1
5 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 965 0
6 NAME Musca Cld 12 23 -71.3           ~ 258 0
7 NGC 6334 HII 17 20 53 -36 07.9           ~ 740 0
8 W 51 SNR 19 23 50 +14 06.0           ~ 1352 1

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