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Open AccessJournal ArticleDOI

Non-hermitian localization and population biology

David R. Nelson, +1 more
- 01 Aug 1998 - 
- Vol. 58, Iss: 2, pp 1383-1403
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TLDR
This work proposes a delocalization transition for the steady state of the nonlinear problem at a critical convection threshold separating localized and extended states, and describes singular scaling behavior described by a $(d\ensuremath{-}1)$-dimensional generalization of the noisy Burgers' equation.
Abstract
The time evolution of spatial fluctuations in inhomogeneous $d$-dimensional biological systems is analyzed A single species continuous growth model, in which the population disperses via diffusion and convection is considered Time-independent environmental heterogeneities, such as a random distribution of nutrients or sunlight are modeled by quenched disorder in the growth rate Linearization of this model of population dynamics shows that the fastest growing localized state dominates in a time proportional to a power of the logarithm of the system size Using an analogy with a Schr\"odinger equation subject to a constant imaginary vector potential, we propose a delocalization transition for the steady state of the nonlinear problem at a critical convection threshold separating localized and extended states In the limit of high convection velocity, the linearized growth problem in $d$ dimensions exhibits singular scaling behavior described by a $(d\ensuremath{-}1)$-dimensional generalization of the noisy Burgers' equation, with universal singularities in the density of states associated with disorder averaged eigenvalues near the band edge in the complex plane The Burgers mapping leads to unusual transverse spreading of convecting delocalized populations

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Citations
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PT-symmetric quantum mechanics

TL;DR: In this paper, the authors proposed a generalization of Hermiticity for complex deformation H =p2+x2(ix)e of the harmonic oscillator Hamiltonian, where e is a real parameter.
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Exceptional topology of non-Hermitian systems

TL;DR: In this paper, the role of topology in non-Hermitian (NH) systems and its far-reaching physical consequences observable in a range of dissipative settings are reviewed.
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Topological phases of non-Hermitian systems

TL;DR: In this article, a coherent framework of topological phases of non-Hermitian Hamiltonians was developed, and the K-theory was applied to systematically classify all the topology phases in the Altland-Zirnbauer classes in all dimensions.
Journal ArticleDOI

Topological Phases of Non-Hermitian Systems

TL;DR: In this paper, a coherent framework of topological phases of non-Hermitian Hamiltonians was developed, and the K-theory was applied to systematically classify all the topology phases in the Altland-Zirnbauer classes in all dimensions.
Journal ArticleDOI

Generalized bulk–boundary correspondence in non-Hermitian topolectrical circuits

TL;DR: In this paper, a non-Hermitian skin effect was observed in a topolectric circuit with respect to the presence of a boundary, and the voltage signal accumulates at the left or right boundary and increases as a function of nodal distance to the current feed.
References
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Book

The Theory of Matrices

TL;DR: In this article, the Routh-Hurwitz problem of singular pencils of matrices has been studied in the context of systems of linear differential equations with variable coefficients, and its applications to the analysis of complex matrices have been discussed.
Book

Linear and Nonlinear Waves

G. B. Whitham
TL;DR: In this paper, a general overview of the nonlinear theory of water wave dynamics is presented, including the Wave Equation, the Wave Hierarchies, and the Variational Method of Wave Dispersion.
Book

Theory of matrices

Journal ArticleDOI

Pattern formation outside of equilibrium

TL;DR: A comprehensive review of spatiotemporal pattern formation in systems driven away from equilibrium is presented in this article, with emphasis on comparisons between theory and quantitative experiments, and a classification of patterns in terms of the characteristic wave vector q 0 and frequency ω 0 of the instability.
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