期刊
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
卷 466, 期 2, 页码 2272-2283出版社
OXFORD UNIV PRESS
DOI: 10.1093/mnras/stw3319
关键词
magnetic fields; MHD; turbulence; methods: data analysis; ISM: structure
资金
- Australian Postgraduate Award
- Vice Chancellor's Research Scholarship - University of Sydney
- Australian Research Council [DP150104329, FT150100024]
- Natural Sciences and Engineering Research Council of Canada (NSERC) [RGPIN-2015-05948]
- NASA Einstein Postdoctoral Fellowship
- Julich Supercomputing Centre [hhd20]
- Gauss Centre for Supercomputing [pr32lo, pr48pi, 10391]
- Partnership for Advanced Computing in Europe (PRACE grant) [pr89mu]
- Australian National Computational Infrastructure [ek9]
- Australian Government
- Government of Western Australia
- Department of Energy (DOE)
Previous studies have shown that star formation depends on the driving of molecular cloud turbulence, and differences in the driving can produce an order of magnitude difference in the star formation rate. The turbulent driving is characterized by the parameter zeta, with zeta = 0 for compressive, curl-free driving (e.g. accretion or supernova explosions), and zeta = 1 for solenoidal, divergence-free driving (e.g. Galactic shear). Here we develop a new method to measure zeta from observations of synchrotron emission from molecular clouds. We calculate statistics of mock synchrotron intensity images produced from magnetohydrodynamic simulations of molecular clouds, in which the driving was controlled to produce different values of zeta. We find that the mean and standard deviation of the log-normalized synchrotron intensity are sensitive to zeta, for values of zeta between 0 (curl-free driving) and 0.5 (naturally mixed driving). We quantify the dependence of zeta on the direction of the magnetic field relative to the line of sight. We provide best-fitting formulae for zeta in terms of the log-normalized mean and standard deviation of synchrotron intensity, with which zeta can be determined for molecular clouds that have similar Alfvenic Mach number to our simulations. These formulae are independent of the sonic Mach number. Signal-to-noise ratios larger than 5, and angular resolutions smaller than 5 per cent of the cloud diameter, are required to apply these formulae. Although there are no firm detections of synchrotron emission from molecular clouds, by combining Green Bank Telescope and Very Large Array observations it should be possible to detect synchrotron emission from molecular clouds, thereby constraining the value of zeta.
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