Abstract

Banded patterns in limestone-marl sequences (“rhythmites”) form widespread sediments typical of shallow marine environments. They are characterized by alternations of limestone-rich layers and softer calcareous-clayey material (marl) extending over hundreds of meters with a thickness of a few tens of meters. The banded sequences are usually thought to result from systematic variations in the external environment, but the pattern may be distorted by diagenetic nonlinear processes. Here, we present a reactive-transport model for the formation of banded patterns in such a system. The model exhibits interesting features typical of nonlinear dynamical systems: (i) the existence of self-organized oscillating patterns between a calcite-rich mode (“limestone”) and a calcite-poor one (“marl”) for fixed environmental conditions and (ii) bistability between these two modes. We then illustrate the phenomena of stochastic resonance, whereby the multistable system is driven by a small external periodic signal (the 100,000 years’ Milankovitch cycle comes to mind) that is too weak to generate oscillations between the states on its own. In the presence of random fluctuations, however, the system generates transitions between the calcite-rich and calcite-poor states in statistical synchrony with the external forcing. The signal-to-noise ratio exhibits many maxima as the noise strength is varied. Hence, this amplification effect is maximized for specific values of the noise strength.

Highlights

  • Rocks and minerals often exhibit rhythmic spatial variations in their chemical and/or physical properties over length scales varying from the micrometer to the kilometer [1,2,3]

  • In a nonlinear nonequilibrium geosystem, the presence of positive feedback may result in a pattern formation that is self-organized even in an external environment that does not change [2, 4]. Examples of such geochemical self-organization are found in the oscillatory zoning of solid solutions series [4, 6,7,8,9], Liesegang band formation [10,11,12,13,14,15,16,17], orbicular granites [7, 18], and cyclic layering in igneous bodies [19, 20]

  • If a random component is included in the external signal, transitions between distinct attractors become possible for sufficiently strong noise strength

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Summary

Introduction

Rocks and minerals often exhibit rhythmic spatial variations in their chemical and/or physical properties over length scales varying from the micrometer to the kilometer [1,2,3]. As a result of burial, a new portion of immature fresh sediment passes through the ADZ and the cycle is ready to start again Through this diagenetic self-organization mechanism, a sequence of cemented calcite-rich layers (limestone) and Aragonite-depleted sediment Cemented sediment Fresh sediment Stationary aragonite dissolution zone (ADZ). We establish the existence of diagenetic self-organization in the model, as well as multistability, that is, long-time asymptotic solutions that are characterized by qualitatively different compositions at the bottom of the sediment layer This invokes the possibility of noiseinduced transitions between the various states.

Deterministic Diagenetic Model
Deterministic Solutions
Stochastic Resonance: A Primer
Stochastic Resonance Applied to the Limestone-Marl Diagenetic Model
Conclusion
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