4.6 Article

High-accuracy estimation of magnetic field strength in the interstellar medium from dust polarization

期刊

ASTRONOMY & ASTROPHYSICS
卷 647, 期 -, 页码 -

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361/202039779

关键词

ISM: magnetic fields; magnetohydrodynamics (MHD); polarization

资金

  1. European Research Council (ERC) under the European Unions Horizon 2020 research and innovation programme [771282]

向作者/读者索取更多资源

The study aims to develop a new method for estimating the magnetic field strength in the interstellar medium, by including compressible modes and accounting for the anisotropic properties of turbulence. A formula is derived based on simple energetics arguments, which takes into account gas density, velocity, and polarization angle dispersion. Synthetic observations from 3D MHD simulations show that the accuracy of the new method is not dependent on the turbulence properties of the simulated model.
Context. A large-scale magnetic field permeates our Galaxy and is involved in a variety of astrophysical processes, such as star formation and cosmic ray propagation. Dust polarization has been proven to be one of the most powerful observables for studying the field properties in the interstellar medium (ISM). However, it does not provide a direct measurement of its strength. Different methods have been developed that employ both polarization and spectroscopic data in order to infer the field strength. The most widely applied method was developed by Davis (1951, Phys. Rev., 81, 890) and Chandrasekhar & Fermi (1953, ApJ, 118, 1137), hereafter DCF. The DCF method relies on the assumption that isotropic turbulent motions initiate the propagation of Alfven waves. Observations, however, indicate that turbulence in the ISM is anisotropic and that non-Alfvenic (compressible) modes may be important.Aims. Our goal is to develop a new method for estimating the field strength in the ISM that includes the compressible modes and does not contradict the anisotropic properties of turbulence.Methods. We adopt the following assumptions: (1) gas is perfectly attached to the field lines; (2) field line perturbations propagate in the form of small-amplitude magnetohydrodynamic (MHD) waves; and (3) turbulent kinetic energy is equal to the fluctuating magnetic energy. We use simple energetics arguments that take the compressible modes into account to estimate the strength of the magnetic field.Results. We derive the following equation: radic B0=, where rho is the gas density, delta v is the rms velocity as derived from the spread of emission lines, and delta theta is the dispersion of polarization angles. We produce synthetic observations from 3D MHD simulations, and we assess the accuracy of our method by comparing the true field strength with the estimates derived from our equation. We find a mean relative deviation of 17%. The accuracy of our method does not depend on the turbulence properties of the simulated model. In contrast, the DCF method, even when combined with the Hildebrand et al. (2009, ApJ, 696, 567) and Houde et al. (2009, ApJ, 706, 1504) method, systematically overestimates the field strength.Conclusions. Compressible modes can significantly affect the accuracy of methods that are based solely on Alfvenic modes. The formula that we propose includes compressible modes; however, it is applicable only in regions with no self-gravity. Density inhomogeneities may bias our estimates to lower values.

作者

我是这篇论文的作者
点击您的名字以认领此论文并将其添加到您的个人资料中。

评论

主要评分

4.6
评分不足

次要评分

新颖性
-
重要性
-
科学严谨性
-
评价这篇论文

推荐

暂无数据
暂无数据