Author:
Mergny Pierre,Majumdar Satya N
Abstract
Abstract
We study the probability of stability of a large complex system of size N within the framework of a generalized May model, which assumes a linear dynamics of each population size n
i
(with respect to its equilibrium value):
d
n
i
d
t
=
−
a
i
n
i
−
T
∑
j
J
i
j
n
j
. The a
i
> 0’s are the intrinsic decay rates, J
ij
is a real symmetric (N × N) Gaussian random matrix and
T
measures the strength of pairwise interaction between different species. Our goal is to study how inhomogeneities in the intrinsic damping rates a
i
affect the stability of this dynamical system. As the interaction strength T increases, the system undergoes a phase transition from a stable phase to an unstable phase at a critical value T = T
c. We reinterpret the probability of stability in terms of the hitting time of the level b = 0 of an associated Dyson Brownian motion (DBM), starting at the initial position a
i
and evolving in ‘time’ T. In the large N → ∞ limit, using this DBM picture, we are able to completely characterize T
c for arbitrary density μ(a) of the a
i
’s. For a specific flat configuration
a
i
=
1
+
σ
i
−
1
N
, we obtain an explicit parametric solution for the limiting (as N → ∞) spectral density for arbitrary T and σ. For finite but large N, we also compute the large deviation properties of the probability of stability on the stable side T < T
c using a Coulomb gas representation.
Subject
Statistics, Probability and Uncertainty,Statistics and Probability,Statistical and Nonlinear Physics
Cited by
8 articles.
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