Abstract

ABSTRACTSince the AD 775 and AD 994 Δ14C peak (henceforth M12) was first measured by Miyake et al. (2012, 2013), several possible production mechanisms for these spike have been suggested, but the work of Mekhaldi et al. (2015) shows that a very soft energy spectrum was involved, implying that a strong solar energetic particle (SEP) event (or series of events) was responsible. Here we present Δ14C values from AD 721–820 Sequoiadendron giganteum annual tree-ring samples from Sequoia National Park in California, USA, together with Δ14C in German oak from 650–670 BC. The AD 721–820 measurements confirm that a sharp Δ14C peak exists at AD 775, with a peak height of approximately 15‰ and show that this spike was preceded by several decades of rapidly decreasing Δ14C. A sharp peak is also present at 660 BC, with a peak height of about 10‰, and published data (Reimer et al. 2013) indicate that it too was preceded by a multi-decadal Δ14C decrease, suggesting that solar activity was very strong just prior to both Δ14C peaks and may be causally related. During periods of strong solar activity there is increased probability for coronal mass ejection (CME) events that can subject the Earth’s atmosphere to high fluencies of solar energetic particles (SEPs). Periods of high solar activity (such as one in October–November 2003) can also often include many large, fast CMEs increasing the probability of geomagnetic storms. In this paper we suggest that the combination of large SEP events and elevated geomagnetic activity can lead to enhanced production of 14C and other cosmogenic isotopes by increasing the area of the atmosphere that is irradiated by high solar energetic particles.

Highlights

  • In this paper we suggest that the combination of large SEP events and elevated geomagnetic activity can lead to enhanced production of 14C and other cosmogenic isotopes by increasing the area of the atmosphere that is irradiated by high solar energetic particles

  • Since the Northern Hemisphere (NH) growing season is generally from April to September, the appearance time of M12 in NH datasets is recorded here as AD 775.5 and if a Southern Hemisphere (SH) tree ring showing M12 grew from October AD 774 to April AD 775, the appearance time of M12 is recorded as AD 775.0 (Güttler et al 2015)

  • The 660 BC rise time is longer than that of M12 and the height is lower, both peaks appear during periods of strong solar activity, and the simplest explanation for the 660 BC and AD 994 spikes and M12 is that all three have a common cause

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Summary

Introduction

The strongest peak of Δ14C, corresponding to the event of AD 775 (called M12), and another peak in AD 993/4 were measured by Miyake (Miyake et al 2012, 2013) using 14C in annually resolved Japanese cedar tree-ring sequences, and M12 has been confirmed by several studies (Usoskin et al 2013; Jull et al 2014; Güttler et al 2015; Rakowski et al 2015; Büntgen et al 2016) including three that showed peaks with slightly different starting times. Since the AD 775 and AD 994 Δ14C peak ( M12) was first measured by Miyake et al (2012, 2013), several possible production mechanisms for these spike have been suggested, but the work of Mekhaldi et al (2015) shows that a very soft energy spectrum was involved, implying that a strong solar energetic particle (SEP) event (or series of events) was responsible.

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