Abstract

The endogenous circadian clock drives oscillations that are completely synchronized with the environmental day–night rhythms with a period of approximately 24 hours. Temporal misalignment between one’s internal circadian clock and the external solar time often occurs in shift workers and long-distance travelers; such misalignments are accompanied by sleep disturbances and gastrointestinal distress. Repeated exposure to jet lag and rotating shift work increases the risk of lifestyle-related diseases, such as cardiovascular complaints and metabolic insufficiencies. However, the mechanism behind the disruption of one’s internal clock is not well understood. In this paper, we therefore present a new theoretical concept called “jet lag separatrix” to understand circadian clock disruption and slow recovery from jet lag based on the mathematical model describing the hierarchical structure of the circadian clock. To demonstrate the utility of our theoretical study, we applied it to predict that re-entrainment via a two-step jet lag in which a four-hour shift of the light-dark cycle is given in the span of two successive days requires fewer days than when given as a single eight-hour shift. We experimentally verified the feasibility of our theory in C57BL/6 strain mice, with results indicating that this pre-exposure of jet lag is indeed beneficial.

Highlights

  • Jet lag can be emulated in laboratory experiments by presenting an abrupt shift of the light-dark (LD) cycle to animals

  • We proposed a mathematical model to investigate the role of intercellular coupling in the suprachiasmatic nucleus (SCN) during the adaptation process after substantial jet lag[14]

  • We expect that the jet lag separatrix should be found in a variety of organisms ranging from single cell organisms to mammals

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Summary

AVP output

Coupling in the SCN, large desynchrony among SCN neurons just after advancing LD cycle, and slow adaptation to the new LD cycle—are closely interrelated. (i) phase dispersion; (ii) jet lag separatrix; (iii) desynchrony and slow re-entrainment for advance phase shifts Each of these properties is described in further detail below. PS50 for various δ values (i.e., the blue symbols in Fig. 3) shows that compared to the case of K2 = 0, the asymmetry between advance and delayed jet lag is further enhanced, and the width of the region of slow adaptation, which is present around δ near δ*, becomes much wider. This occurs because synchronization level R considerably decreases for a substantial amount of time after jet lag in this region of δ

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