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Scientific Report 2007-2009<br />

Astronomy & Astrophysics<br />

A5. Search for periodicities in the solar energetic proton fluxes<br />

Past studies revealed that many solar activity phenomena<br />

undergo both periodic and quasi-periodic variations<br />

on different time scales. Nevertheless, only a few<br />

attempts were made so far to detect corresponding variations<br />

in the occurence frequency of solar energetic particle<br />

events. We tried to fill this gap searching for periodicities<br />

in the proton fluxes, measured in the interplanetary<br />

space, on time scales ranging from a few Bartels rotations<br />

(27 days) up the the Schwabe period (≈11 years).<br />

Figure 1: The wavelet power (normalized to the 95% significant<br />

level) corresponding to the most relevant periods (as<br />

<strong>report</strong>ed in the legend) are plotted as a function of time for<br />

channel P2 (top) and channel P11 (bottom). An upper cutoff<br />

was applied to the data in order to smooth the discontinuities.<br />

Our study was based on the data collected by the<br />

Charged Particle Measurement Experiment (CPME),<br />

aboard the satellite IMP 8, orbiting at ≈35 Earth radii in<br />

the period from 1974 to 2001. Measurements were performed<br />

in ten differential energy channels, but we used<br />

only those taken in channels P2 (0.50 - 0.96 MeV) and<br />

P11 (190 - 440 MeV), which were not affected by an<br />

experiment malfunction occurred in 1989. Data were<br />

analyzed using the wavelet transform (WT), a technique<br />

which offers an important advantage with respect to the<br />

Fourier transform, because it allows localization in time<br />

of possible periodicities which are not present continuously<br />

in the data set. It is known, however, that the<br />

WT may lead to erroneus results, when applied to discontinuous<br />

data, such as the proton fluxes considered in<br />

our study. We investigated this issue by applying the<br />

wavelet analysis to suitable test functions. It turned out<br />

that eventual spurious frequencies can be discarded by<br />

introducing an upper cutoff to reduce the amplitude of<br />

the stronger discontinuities present in the data set.<br />

Discarded the spurious periods, our analysis revealed<br />

variations of the proton fluxes on the following time<br />

scales (see Figure 1):<br />

T = 3.8 years. This period has been singled out in<br />

both the energy channels from 1977 to 1985 (the active<br />

phase of solar cycle 21). It closely resembles the 3.7 year<br />

period exhibited by the protospheric magnetic field in<br />

the same time interval.<br />

T = 1.7 - 2.2 years. This modulation, also present in<br />

both the energy channels, is better observed from 1988<br />

to 1993 (i.e., around the sunspot maximum of the cycle<br />

22). It corresponds to the ”quasi biennial oscillations”<br />

(QBO) which are known to characterize several features<br />

of the solar activity: e.g., the number of H flares, the<br />

total sunspot area, the 10.7 cm radio emission, and the<br />

flux of the energetic electrons. The common origin of<br />

all these phenomena is supported by the simultaneous<br />

disappearance of their modulation during quiet periods.<br />

T = 0.8 - 0.9 years. This modulation is observed in<br />

shorter time intervals: its linkage with the variations of<br />

other solar parameters deserves other studies.<br />

We also note the lack, in our data set, of significant<br />

modulations on time scales of 150 days and 5 - 6<br />

years. However, the 150 day period (the so called ”Rieger<br />

period”), revealed in several solar activity parameters,<br />

could have been hardly singled out in our analysis, as<br />

the proton fluxes were averaged over Bartels rotations<br />

(27 days). On the other hand, the absence of the 5.5<br />

year modulation appear to be more significant. In fact<br />

it supports the hypothesis, advanced by some author,<br />

that this periodicity, observed, e.g., in the sunspot number,<br />

is an artifact produced by the asymmetric shape of<br />

the solar cycle.<br />

We finally stress that the procedure we successfully<br />

introduced here to discard spurious periodicities may<br />

be useful when the WT is applied to other sets of data<br />

with strong discontinuities.<br />

References<br />

1. M. Lorenza, et al., Journ. Geophys. Res. 114, A01103,<br />

(2009)<br />

2. M. Storini, et al., Adv. Space Res. 41, 70 (2008).<br />

Authors<br />

G. Moreno<br />

<strong>Sapienza</strong> Università di Roma 152 Dipartimento di Fisica

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