Disorder to Order Transition in 1D non-reciprocal Cahn-Hilliard Model

We present the phenomenology of the one dimensional non-reciprocal Cahn Hilliard model for varying non-reciprocity $(α)$ and different boundary conditions. At small $α$, a perturbed uniform state evolves to a defect laden configuration that lacks global polar order. Defects are the sources and sinks of travelling waves. For a given $α$, defects with a unique wave number that increases monotonically with $α$ are selected. A critical threshold $α_c$ marks the onset of a transition to states with finite global polar order. For periodic boundary conditions, above $α_c$, the system shows travelling waves that are completely ordered. In contrast, travelling waves are incompatible with the Neumann and Dirichlet boundary conditions. Instead, for $α\gtrsim α_c$, we find fluctuating domains that show intermittent polar order and at large $α$, the system partitions into two domains with opposite polar order.

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ArXiv.org
Published
2025-10-13
Primary Topic
Solidification and crystal growth phenomena
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article

Disorder to Order Transition in 1D non-reciprocal Cahn-Hilliard Model

ArXiv.org
Solidification and crystal growth phenomena
article

Disorder to Order Transition in 1D non-reciprocal Cahn-Hilliard Model

article en

Abstract

We present the phenomenology of the one dimensional non-reciprocal Cahn Hilliard model for varying non-reciprocity $(α)$ and different boundary conditions. At small $α$, a perturbed uniform state evolves to a defect laden configuration that lacks global polar order. Defects are the sources and sinks of travelling waves. For a given $α$, defects with a unique wave number that increases monotonically with $α$ are selected. A critical threshold $α_c$ marks the onset of a transition to states with finite global polar order. For periodic boundary conditions, above $α_c$, the system shows travelling waves that are completely ordered. In contrast, travelling waves are incompatible with the Neumann and Dirichlet boundary conditions. Instead, for $α\gtrsim α_c$, we find fluctuating domains that show intermittent polar order and at large $α$, the system partitions into two domains with opposite polar order.

ArXiv.org
Openalex Percentile: Top 58%
Solidification and crystal growth phenomena
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Disorder to Order Transition in 1D non-reciprocal Cahn-Hilliard Model · ArXiv.org (2025) | TGRS Research Map | TGRS