Publication:
Cosmic-Ray Diffusion Coefficients throughout the Inner Heliosphere from a Global Solar Wind Simulation

dc.contributor.authorR. Chhiberen_US
dc.contributor.authorP. Subedien_US
dc.contributor.authorA. V. Usmanoven_US
dc.contributor.authorW. H. Matthaeusen_US
dc.contributor.authorD. Ruffoloen_US
dc.contributor.authorM. L. Goldsteinen_US
dc.contributor.authorT. N. Parasharen_US
dc.contributor.otherBartol Research Instituteen_US
dc.contributor.otherNASA Goddard Space Flight Centeren_US
dc.contributor.otherMahidol Universityen_US
dc.date.accessioned2018-12-21T07:27:05Z
dc.date.accessioned2019-03-14T08:03:29Z
dc.date.available2018-12-21T07:27:05Z
dc.date.available2019-03-14T08:03:29Z
dc.date.issued2017-06-01en_US
dc.description.abstractWe use a three-dimensional magnetohydrodynamic simulation of the solar wind to calculate cosmic-ray diffusion coefficients throughout the inner heliosphere (2 R⊙ - 3 au). The simulation resolves large-scale solar wind flow, which is coupled to small-scale fluctuations through a turbulence model. Simulation results specify background solar wind fields and turbulence parameters, which are used to compute diffusion coefficients and study their behavior in the inner heliosphere. The parallel mean free path (mfp) is evaluated using quasi-linear theory, while the perpendicular mfp is determined from nonlinear guiding center theory with the random ballistic interpretation. Several runs examine varying turbulent energy and different solar source dipole tilts. We find that for most of the inner heliosphere, the radial mfp is dominated by diffusion parallel to the mean magnetic field; the parallel mfp remains at least an order of magnitude larger than the perpendicular mfp, except in the heliospheric current sheet, where the perpendicular mfp may be a few times larger than the parallel mfp. In the ecliptic region, the perpendicular mfp may influence the radial mfp at heliocentric distances larger than 1.5 au; our estimations of the parallel mfp in the ecliptic region at 1 au agree well with the Palmer "consensus" range of 0.080.3 au. Solar activity increases perpendicular diffusion and reduces parallel diffusion. The parallel mfp mostly varies with rigidity (P) as P.33, and the perpendicular mfp is weakly dependent on P. The mfps are weakly influenced by the choice of long-wavelength power spectra.en_US
dc.identifier.citationAstrophysical Journal, Supplement Series. Vol.230, No.2 (2017)en_US
dc.identifier.doi10.3847/1538-4365/aa74d2en_US
dc.identifier.issn00670049en_US
dc.identifier.other2-s2.0-85021373465en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/20.500.14594/42442
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85021373465&origin=inwarden_US
dc.subjectEarth and Planetary Sciencesen_US
dc.titleCosmic-Ray Diffusion Coefficients throughout the Inner Heliosphere from a Global Solar Wind Simulationen_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85021373465&origin=inwarden_US

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