2010
DOI: 10.1016/j.asr.2009.09.005
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Modeling and data analysis of a Forbush decrease

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Cited by 57 publications
(51 citation statements)
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“…Mean value of α for the phase of decrease is about -0.72±0.43, for the phase of minimum about -0.91±0.36, and for the phase of recovery about -0.90±0.51 (RMS deviations are indicated). From the obtained distributions, a conclusion follows that no significant difference between α values for different FD phases is observed, in contradiction with results [7].…”
Section: Results Of Studying Of Fd Characteristics In Muon Fluxcontrasting
confidence: 55%
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“…Mean value of α for the phase of decrease is about -0.72±0.43, for the phase of minimum about -0.91±0.36, and for the phase of recovery about -0.90±0.51 (RMS deviations are indicated). From the obtained distributions, a conclusion follows that no significant difference between α values for different FD phases is observed, in contradiction with results [7].…”
Section: Results Of Studying Of Fd Characteristics In Muon Fluxcontrasting
confidence: 55%
“…A similar study using data of neutron monitors and a muon telescope was carried out earlier [7]. The index of the energy spectrum of decreases was estimated from the URAGAN data with increments of 40-60 minutes.…”
Section: Methods Of Fd Analysis In the Flux Of Muons Registered In Thementioning
confidence: 99%
“…This relationship is expected owing to the dependence of the diffusion coefficient K of GCR particles on the rigidity R, K ∝ R α ; here the coefficient α depends on the exponent ν of the PSD of the IMF turbulence according to the quasi-linear theory (QLT) as α = 2 -ν (Jokipii, 1966(Jokipii, , 1971Hasselman and Wibberentz, 1968;Toptygin, 1985). As was shown by Wawrzynczak and Alania (2005a, 2005b, Wawrzynczak (2008, 2012), and Alania, Iskra, andSiluszyk (2008, 2010), the exponent γ is related to α. Namely, γ ≈ 2 -ν in the range of frequency of the IMF turbulence f ≈ ∼ 10 −6 -10 −5 Hz, to which the neutron monitors and muon telescopes respond. The validity of the QLT (Jokipii, 1966(Jokipii, , 1971 for the GCR particles with energy ≥ 1 GeV is confirmed by the weakly nonlinear theory (WNLT; Shalchi et al, 2004), nonlinear parallel diffusion theory (NLPA; Qin, 2007) and by Droge (2003), Shalchi andSchlickeiser (2004), andShalchi (2009).…”
Section: Introductionmentioning
confidence: 97%
“…However, to study the rigidity dependence of Fd based only on the rigidity spectrum taken at one time point is not sufficient to understand its dynamics. The time evolution of the rigidity spectrum of the Fd was studied by Wawrzynczak (2008, 2012) and by Wawrzynczak and Alania (2005a, 2005b. They showed that the rigidity spectrum δD(R)/D(R) ∝ R −γ of the great majority of Fds gradually becomes hard during the decreasing and minimum phases and then gradually becomes soft in the recovery phase.…”
Section: Introductionmentioning
confidence: 99%
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