@Article{KozaiMKKSDSBMASDHEST:2016:GlMuDe,
author = "Kozai, M. and Munakata, K. and Kato, C. and Kuwabara, T. and
Silva, Marlos Rockenbach da and Dal Lago, Alisson and Schuch,
Nelson Jorge and Braga, Carlos Roberto and Mendon{\c{c}}a, Rafael
Rodrigues Souza de and Al Jassar, H. K. and Sharma, M. M. and
Duldig, M. L. and Humble, J. E. and Evenson, P. and Sabbah, I. and
Tokumaru, M.",
affiliation = "{Shinshu University} and {Shinshu University} and {Shinshu
University} and {Chiba University} and {Instituto Nacional de
Pesquisas Espaciais (INPE)} and {Instituto Nacional de Pesquisas
Espaciais (INPE)} and {Instituto Nacional de Pesquisas Espaciais
(INPE)} and {Instituto Nacional de Pesquisas Espaciais (INPE)} and
{Instituto Nacional de Pesquisas Espaciais (INPE)} and {Kuwait
University} and {Kuwait University} and {University of Tasmania}
and {University of Tasmania} and {University of Delaware} and
{College of Health Sciences} and {Nagoya University}",
title = "Average spatial distribution of cosmic rays behind the
interplanetary shock - Global muon detector network observations",
journal = "Astrophysical Journal",
year = "2016",
volume = "825",
number = "2",
pages = "100",
month = "July",
keywords = "astroparticle physics, cosmic rays, interplanetary medium,
methods: data analysis, solar wind, Sun: coronal mass ejections
(CMEs).",
abstract = "We analyze the galactic cosmic ray (GCR) density and its spatial
gradient in Forbush Decreases (FDs) observed with the Global Muon
Detector Network (GMDN) and neutron monitors (NMs). By superposing
the GCR density and density gradient observed in FDs following 45
interplanetary shocks (IP-shocks), each associated with an
identified eruption on the Sun, we infer the average spatial
distribution of GCRs behind IP-shocks. We find two distinct
modulations of GCR density in FDs, one in the magnetic sheath and
the other in the coronal mass ejection (CME) behind the sheath.
The density modulation in the sheath is dominant in the western
flank of the shock, while the modulation in the CME ejecta stands
out in the eastern flank. This east-west asymmetry is more
prominent in GMDN data responding to \∼60 GV GCRs than in
NM data responding to \∼10 GV GCRs, because of the softer
rigidity spectrum of the modulation in the CME ejecta than in the
sheath. The geocentric solar ecliptic-y component of the density
gradient, G y, shows a negative (positive) enhancement in FDs
caused by the eastern (western) eruptions, while G z shows a
negative (positive) enhancement in FDs caused by the northern
(southern) eruptions. This implies that the GCR density minimum is
located behind the central flank of IP-shocks and propagating
radially outward from the location of the solar eruption. We also
confirmed that the average G z changes its sign above and below
the heliospheric current sheet, in accord with the prediction of
the drift model for the large-scale GCR transport in the
heliosphere.",
doi = "10.3847/0004-637X/825/2/100",
url = "http://dx.doi.org/10.3847/0004-637X/825/2/100",
issn = "0004-637X and 1538-4357",
language = "en",
urlaccessdate = "27 abr. 2024"
}