# Browsing by Subject "modulation equation"

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Item Open Access BIFURCATIONS IN A MODULATION EQUATION FOR ALTERNANS IN A CARDIAC FIBER(ESAIM-MATHEMATICAL MODELLING AND NUMERICAL ANALYSIS-MODELISATION MATHEMATIQUE ET ANALYSE NUMERIQUE, 2010) Dai, S; Schaeffer, DGItem Open Access Bifurcations in the Echebarria-Karma Modulation Equation for Cardiac Alternans in One Dimension(2009) Dai, ShuWhile alternans in a single cardiac cell appears through a simple

period-doubling bifurcation, in extended tissue the exact nature

of the bifurcation is unclear. In particular, the phase of

alternans can exhibit wave-like spatial dependence, either

stationary or traveling, which is known as discordant

alternans. We study these phenomena in simple cardiac models

through a modulation equation proposed by Echebarria-Karma. In

this dissertation, we perform bifurcation analysis for their

modulation equation.

Suppose we have a cardiac fiber of length l, which is

stimulated periodically at its x=0 end. When the pacing period

(basic cycle length) B is below some critical value B

_{c},alternans emerges along the cable. Let a(x,n) be the amplitude

of the alternans along the fiber corresponding to the n-th

stimulus. Echebarria and Karma suppose that a(x,n) varies

slowly in time and it can be regarded as a time-continuous

function a(x,t). They derive a weakly nonlinear modulation

equation for the evolution of a(x,t) under some approximation,

which after nondimensionization is as follows:

&partial

_{t}a = σ a + L a - g a 3,where the linear operator

L a = &partial

_{xx}a - &partial_{x}a -Λ-1 ∫ 0_{x}a(x',t)dx'.In the equation, σ is dimensionless and proportional to

B

_{c}- B, i.e. σ indicates how rapid the pacing is,Λ-1 is related to the conduction velocity (CV) of the

propagation and the nonlinear term -ga3 limits growth after the

onset of linear instability. No flux boundary conditions are

imposed on both ends.

The zero solution of their equation may lose stability, as the

pacing rate is increased. To study the bifurcation, we calculate

the spectrum of operator L. We find that the

bifurcation may be Hopf or steady-state. Which bifurcation occurs

first depends on parameters in the equation, and for one critical

case both modes bifurcate together at a degenerate (codimension 2)

bifurcation.

For parameters close to the degenerate case, we investigate the

competition between modes, both numerically and analytically. We

find that at sufficiently rapid pacing (but assuming a 1:1

response is maintained), steady patterns always emerge as the only

stable solution. However, in the parameter range where Hopf

bifurcation occurs first, the evolution from periodic solution

(just after the bifurcation) to the eventual standing wave

solution occurs through an interesting series of secondary

bifurcations.

We also find that for some extreme range of parameters, the

modulation equation also includes chaotic solutions. Chaotic waves

in recent years has been regarded to be closely related with

dreadful cardiac arrhythmia. Proceeding work illustrated some

chaotic phenomena in two- or three-dimensional space, for instance

spiral and scroll waves. We show the existence of chaotic waves in

one dimension by the Echebarria-Karma modulation equation for

cardiac alternans. This new discovery may provide a different

mechanism accounting for the instabilities in cardiac dynamics.