TITLE: Isolated Versus Non-Isolated Fixed Point, 2D Dynamics
QUESTION [5 upvotes]: I am trying to understand the classification of fixed points in a dynamical systems context (fixed points of a system of two linear differential equations are places where both $x_1' = x_2' = 0$).
Representing 2D systems as a matrix equation $\vec x'=\matrix A\vec x$, Strogatz classifies fixed points based on $\tau$, the trace of the matrix and $\Delta$, the determinant of the matrix:

unstable node:                                                 $\tau>\sqrt{4\Delta}$,      $\Delta>0$
unstable spiral (spiral source):    $\sqrt{4\Delta}>\tau>0$,              $\Delta>0$
neutrally stable centers:                                $\tau=0$,              $\Delta>0$
stable spiral (spiral sink):          $-\sqrt{4\Delta}<\tau<0$,             $\Delta>0$
stable node:                                                      $\tau<-\sqrt{4\Delta}$,  $\Delta>0$
saddle point:                                                                              $\Delta<0$

However, he is very vague about the boundary cases.  Specifically, what happens on the parabola $\tau^2-4\Delta=0$ and the line $\Delta=0$?
Strogatz mentions that these include star nodes (decoupled systems), degenerate nodes (one unique eigendirection), and nonisolating fixed points.  However, in a later problem, he mentions "isolating fixed points".  What is the difference?
How are all of these nonstandard edge cases classified in terms of $\tau$ and $\Delta$?

REPLY [8 votes]: An isolated fixed point means that one can construct a region around the fixed point such that no other fixed points lie within.  A nonisolated fixed point is the converse (i.e. there are other fixed points arbitrarily close; in practice, these end up being lines or a plane of fixed points).
As far as classification:
For 2D linear systems (or for linearization predictions concerning 2D nonlinear systems):

if $\Delta<0$:
Isolated fixed pointCASE #1: Saddle Point
if $\Delta=0$:
Nonisolated fixed points

if $\tau<0$:
CASE #2: Line of Ляпуно́в (Lyapunov) stable fixed points
if $\tau=0$:
CASE #3: Plane of fixed points
if $\tau>0$:
CASE #4: Line of unstable fixed points

if $\Delta>0$:
Isolated fixed point

if $\tau<-\sqrt{4\Delta}$:
CASE #5: Stable Node
if $\tau=-\sqrt{4\Delta}$:

if there are no uniquely determined eigenvectors (both can be anything):
CASE #6: Stable Star
if there is one uniquely determined eigenvector (the other can be anything):
CASE #7: Stable Degenerate Node

if $-\sqrt{4\Delta}<\tau<0$:
CASE #8: Stable Spiral
if $\tau=0$:
CASE #9: Stable Center
if $0<\tau<\sqrt{4\Delta}$:
CASE #10: Unstable Spiral
if $\tau=\sqrt{4\Delta}$:

if there are no uniquely determined eigenvectors (both can be anything):
CASE #11: Unstable Star
if there is one uniquely determined eigenvector (the other can be anything):
CASE #12: Unstable Degenerate Node

if $\sqrt{4\Delta}<\tau$:
CASE #13: Unstable Node


General Notes:

For 2D linear systems, the above predictions are always accurate.
For 2D nonlinear systems, when the above are used as predictions:

The descriptions are always correct for cases #1, #5, #8, #10, and #13 but can be inaccurate for cases #2, #3, #4, #6, #7, #9, #11, and #12.
Ambiguous cases #6, #7, #11, and #12 at least have their stability correctly determined.
If the system is conservative, a prediction of case #9 is accurate.