# Hopf bifurcation

In the mathematical theory of bifurcations, a Hopf bifurcation is a critical point where a system's stability switches and a periodic solution arises.[1] More accurately, it is a local bifurcation in which a fixed point of a dynamical system loses stability, as a pair of complex conjugate eigenvalues (of the linearization around the fixed point) cross the complex plane imaginary axis. Under reasonably generic assumptions about the dynamical system,a small-amplitude limit cycle branches from the fixed point.

A Hopf bifurcation is also known as a Poincaré–Andronov–Hopf bifurcation, named after Henri Poincaré, Eberhard Hopf, and Aleksandr Andronov.

## Overview

### Supercritical and subcritical Hopf bifurcations

The limit cycle is orbitally stable if a specific quantity called the first Lyapunov coefficient is negative, and the bifurcation is supercritical. Otherwise it is unstable and the bifurcation is subcritical.

The normal form of a Hopf bifurcation is:

${\displaystyle {\frac {dz}{dt}}=z((\lambda +i)+b|z|^{2}),}$

where zb are both complex and λ is a parameter. Write

${\displaystyle b=\alpha +i\beta .\,}$

The number α is called the first Lyapunov coefficient.

• If α is negative then there is a stable limit cycle for λ > 0:
${\displaystyle z(t)=re^{i\omega t}\,}$
where
${\displaystyle r={\sqrt {-\lambda /\alpha }}{\text{ and }}\omega =1+\beta r^{2}.\,}$
The bifurcation is then called supercritical.
• If α is positive then there is an unstable limit cycle for λ < 0. The bifurcation is called subcritical.

### Remarks

The "smallest chemical reaction with Hopf bifurcation" was found in 1995 in Berlin, Germany.[2] The same biochemical system has been used in order to investigate how the existence of a Hopf bifurcation influences our ability to reverse-engineer dynamical systems.[3]

Under some general hypothesis, in the neighborhood of a Hopf bifurcation, a stable steady point of the system gives birth to a small stable limit cycle. Remark that looking for Hopf bifurcation is not equivalent to looking for stable limit cycles. First, some Hopf bifurcations (e.g. subcritical ones) do not imply the existence of stable limit cycles; second, there may exist limit cycles not related to Hopf bifurcations.

### Example

The Hopf bifurcation in the Selkov system (see article). As the parameters change, a limit cycle (in blue) appears out of an unstable equilibrium.

Hopf bifurcations occur in the Hodgkin–Huxley model for nerve membrane,[4] the Selkov model[5] of glycolysis, the Belousov–Zhabotinsky reaction, the Lorenz attractor and in the following simpler chemical system called the Brusselator as the parameter B changes:

${\displaystyle {\frac {dX}{dt}}=A+X^{2}Y-(B+1)X}$
${\displaystyle {\frac {dY}{dt}}=BX-X^{2}Y.}$

The Selkov model is

${\displaystyle {\frac {dx}{dt}}=-x+ay+x^{2}y,~~{\frac {dy}{dt}}=b-ay-x^{2}y.}$

The phase portrait illustrating the Hopf bifurcation in the Selkov model is shown on the right. See Strogatz, Steven H. (1994). "Nonlinear Dynamics and Chaos",[6] page 205 for detailed derivation.

## Definition of a Hopf bifurcation

The appearance or the disappearance of a periodic orbit through a local change in the stability properties of a steady point is known as the Hopf bifurcation. The following theorem works with steady points with one pair of conjugate nonzero purely imaginary eigenvalues. It tells the conditions under which this bifurcation phenomenon occurs.

Theorem (see section 11.2 of [7]). Let ${\displaystyle J_{0}}$ be the Jacobian of a continuous parametric dynamical system evaluated at a steady point ${\displaystyle Z_{e}}$ of it. Suppose that all eigenvalues of ${\displaystyle J_{0}}$ have negative real parts except one conjugate nonzero purely imaginary pair ${\displaystyle \pm i\beta }$. A Hopf bifurcation arises when these two eigenvalues cross the imaginary axis because of a variation of the system parameters.

## Routh–Hurwitz criterion

Routh–Hurwitz criterion (section I.13 of [8]) gives necessary conditions so that a Hopf bifurcation occurs. Let us see how one can use concretely this idea.[9]

### Sturm series

Let ${\displaystyle p_{0},p_{1},\dots ,p_{k}}$ be Sturm series associated to a characteristic polynomial ${\displaystyle P}$. They can be written in the form:

${\displaystyle p_{i}(\mu )=c_{i,0}\mu ^{k-i}+c_{i,1}\mu ^{k-i-2}+c_{i,2}\mu ^{k-i-4}+\cdots }$

The coefficients ${\displaystyle c_{i,0}}$ for ${\displaystyle i}$ in ${\displaystyle \{1,\dots ,k\}}$ correspond to what is called Hurwitz determinants.[9] Their definition is related to the associated Hurwitz matrix.

### Propositions

Proposition 1. If all the Hurwitz determinants ${\displaystyle c_{i,0}}$ are positive, apart perhaps ${\displaystyle c_{k,0}}$ then the associated Jacobian has no pure imaginary eigenvalues.

Proposition 2. If all Hurwitz determinants ${\displaystyle c_{i,0}}$ (for all ${\displaystyle i}$ in ${\displaystyle \{0,\dots ,k-2\}}$ are positive, ${\displaystyle c_{k-1,0}=0}$ and ${\displaystyle c_{k-2,1}<0}$ then all the eigenvalues of the associated Jacobian have negative real parts except a purely imaginary conjugate pair.

The conditions that we are looking for so that a Hopf bifurcation occurs (see theorem above) for a parametric continuous dynamical system are given by this last proposition.

## Example

Let us consider the classical Van der Pol oscillator written with ordinary differential equations:

${\displaystyle \left\{{\begin{array}{l}{\dfrac {dx}{dt}}=\mu (1-y^{2})x-y,\\{\dfrac {dy}{dt}}=x.\end{array}}\right.}$

The Jacobian matrix associated to this system follows:

${\displaystyle J={\begin{pmatrix}-\mu (-1+y^{2})&-2\mu yx-1\\1&0\end{pmatrix}}.}$

The characteristic polynomial (in ${\displaystyle \lambda }$) of the linearization at (0,0) is equal to:

${\displaystyle P(\lambda )=\lambda ^{2}-\mu \lambda +1.}$

The coefficients are: ${\displaystyle a_{0}=1,a_{1}=-\mu ,a_{2}=1}$
The associated Sturm series is:

${\displaystyle {\begin{array}{l}p_{0}(\lambda )=a_{0}\lambda ^{2}-a_{2}\\p_{1}(\lambda )=a_{1}\lambda \end{array}}}$

The Sturm polynomials can be written as (here ${\displaystyle i=0,1}$):

${\displaystyle p_{i}(\mu )=c_{i,0}\mu ^{k-i}+c_{i,1}\mu ^{k-i-2}+c_{i,2}\mu ^{k-i-4}+\cdots }$

The above proposition 2 tells that one must have:

${\displaystyle c_{0,0}=1>0,c_{1,0}=-\mu =0,c_{0,1}=-1<0.}$

Because 1 > 0 and −1 < 0 are obvious, one can conclude that a Hopf bifurcation may occur for Van der Pol oscillator if ${\displaystyle \mu =0}$.

## References

1. ^ "Hopf Bifurcations." (PDF). MIT.
2. ^ Wilhelm, T.; Heinrich, R. (1995). "Smallest chemical reaction system with Hopf bifurcation". Journal of Mathematical Chemistry. 17 (1): 1–14. doi:10.1007/BF01165134.
3. ^ Kirk, P. D. W.; Toni, T.; Stumpf, M. P. H. (2008). "Parameter inference for biochemical systems that undergo a Hopf bifurcation" (PDF). Biophysical Journal. 95 (2): 540–549. doi:10.1529/biophysj.107.126086. PMC . PMID 18456830.
4. ^ Guckenheimer, J.; Labouriau, J.S. (1993), "Bifurcation of the Hodgkin and Huxley equations: A new twist", Bulletin of Mathematical Biology, 55 (5): 937–952, doi:10.1007/BF02460693.
5. ^ "Selkov Model Wolfram Demo". [demonstrations.wolfram.com ]. Retrieved 30 September 2012.
6. ^ Strogatz, Steven H. (1994). Nonlinear Dynamics and Chaos. Addison Wesley publishing company.
7. ^ Hale, J.; Koçak, H. (1991). Dynamics and Bifurcations. Texts in Applied Mathematics. 3. New York: Springer-Verlag.
8. ^ Hairer, E.; Norsett, S. P.; Wanner, G. (1993). Solving ordinary differential equations I: nonstiff problems (Second ed.). New York: Springer-Verlag.
9. ^ a b Kahoui, M. E.; Weber, A. (2000). "Deciding Hopf bifurcations by quantifier elimination in a software component architecture". Journal of Symbolic Computation. 30 (2): 161–179. doi:10.1006/jsco.1999.0353.