J/A+A/587/A150      Solar activity during the Holocene       (Usoskin+, 2016)

Solar activity during the Holocene: the Hallstatt cycle and its consequence for grand minima and maxima. Usoskin I.G., Gallet Y., Lopes F., Kovaltsov G.A., Hulot G. <Astron. Astrophys. 587, A150 (2016)> =2016A&A...587A.150U 2016A&A...587A.150U (SIMBAD/NED BibCode)
ADC_Keywords: Sun Keywords: Sun: activity - solar-terrestrial relations Abstract: Cosmogenic isotopes provide the only quantitative proxy to analyze the long-term solar variability over the centennial time scale. While an essential progress has been achieved in both measurements and modelling of the cosmogenic proxy, uncertainties still remain in the determination of the geomagnetic dipole moment evolution. Here we aim at improving the reconstruction of solar activity over the past nine millennia using a multi-proxy approach. We use records of the 14C and 10Be cosmogenic isotopes, up-to-date numerical models of the isotope production and transport in the Earth's atmosphere, and available geomagnetic field reconstructions, including a new reconstruction relying on an updated archeo/paleointensity database. The obtained series were analyzed using the SSA (Singular Spectrum Analysis) method to study the millennial-scale trends. A new reconstruction of the geomagnetic dipole field moment, referred to as GMAG.9k, is built for the last nine millennia. New reconstructions of solar activity covering the last nine millennia, quantified in terms of sunspot numbers, are presented and analyzed. A conservative list of Grand minima and maxima is also provided. The primary components of the reconstructed solar activity, as determined using the SSA method, are different for the 14C and 10Be based series. This shows that these primary components can only be ascribed to long-term changes in the terrestrial system, and not to the Sun. These components have therefore been removed from the reconstructed series. In contrast, the secondary SSA components of the reconstructed solar activity are found to be dominated by a common ∼2400-year quasi-periodicity, the so-called Hallstatt cycle, in both the 14C and 10Be based series. This Hallstatt cycle thus appears to be related to solar activity. Finally, it is shown that the Grand minima and Grand maxima occurred intermittently over the studied period, with clustering near highs and lows of the Hallstatt cycle, respectively. Description: tables1.dat contains axial dipole evolution between 1500 BC and 1900 AD as constrained by Virtual Axial Dipole Moments (VADM) averaged over sliding windows of 200 years shifted every 10 years. tables2.dat contains axial dipole evolution between 6750 BC and 1500 BC as constrained by Virtual Axial Dipole Moments (VADM) averaged over sliding windows of 500 years shifted every 10 years. Details on the computations are provided in Appendix A. The columns report the epoch [yr], the mean VADM [Gmean] (in units of 1022 Am2), the standard deviation [SD] and the maximum [Gmax] and minimum [Gmin] values defining the envelope of possible VADM results. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tables1.dat 41 341 Virtual Dipole Moment (VDM) for 1500 BC - 1900 AD tables2.dat 41 526 Virtual Dipole Moment (VDM) for 6750 BC - 1500 BC -------------------------------------------------------------------------------- See also: J/A+A/531/A6 : Evolution of solar irradiance during Holocene (Vieira+, 2011) Byte-by-byte Description of file: tables1.dat tables2.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 7 F7.1 yr Year Year AD ("-" denotes years BC) 9- 15 F7.4 10+22A*m+2 Gmean Mean Virtual Axial Dipole Moment (VADM) 18- 25 F8.6 10+22A*m+2 SD Standard deviation of VADM 27- 33 F7.4 10+22A*m+2 Gmax Maximum Virtual Axial Dipole Moment 35- 41 F7.4 10+22A*m+2 Gmin Minimum Virtual Axial Dipole Moment -------------------------------------------------------------------------------- Acknowledgements: Ilya Usoskin, ilya.usoskin(at)oulu.fi Yves Gallet, gallet(at)ipgp.fr
(End) Patricia Vannier [CDS] 18-Jan-2016
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