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Dynamics of flows and maps (continuous and discrete time), including infinite-dimensional dynamics, Hamiltonian dynamics, ergodic theory.
6
votes
Accepted
Nontrivial extension of the action of complex hyperbolic group $H$ on $\mathbb{C}$
The group $H$ acts transitively and primitively on $\mathbb{C}=\mathbb{R}^2$. ('Primitive' means that $H$ preserves no nontrivial foliation.) It's a consequence of the classification of transitive pr …
3
votes
Equivalence problem of classifying heat equations
I'll just add a few more references to what Ben McKay mentioned.
Phillip Griffiths and I wrote a paper on invariants of parabolic equations in 1 space variable (Characteristic cohomology of differenti …
8
votes
Accepted
A vector field whose flow has constant singular values
The vector fields $X$ that satisfy this condition are highly constrained, as there exist only a finite-dimensional family of $C^5$ solutions in a neighborhood of any given point in the plane. Here is …
6
votes
A second order nonlinear ODE
This ODE has some very interesting properties. If one clears fractions and writes it out as
$$
x(x+2y)(x-2y+1)\,y'' = (4x^2-8y^2+3x+4y)\,y' + x(4y-1)\,(y')^2,
\tag1
$$
one recognizes this as the equa …
6
votes
Metrics on torus without closed contractible geodesics
This is a comment, not an answer, but it's too long to fit into a comment window.
I don't know of a 'generic' condition on metrics on the torus that would guarantee that there are no null-homotopic c …
8
votes
Accepted
Complementary integrable vector fields
Actually, it's easier than the general curvature case: Let $X^\flat$ be the $1$-form dual to $X$ via the metric $g$. Then the orthogonal plane field to the integral curves of $X$ is integrable if an …
14
votes
Accepted
Is it possible to prove unboundedness of 3rd order ODE?
Actually, no matter what $A$ is, there will be nonzero solutions that will converge to zero, so you can't prove unboundedness, even though it may be true that the 'generic' solution is unbounded. Her …
10
votes
Accepted
A cubic system with two nested limit cycles with opposite orientations
It is not hard to concoct such an example in sufficiently high degree. For an example of degree $5$, take
$$
\begin{align}
x' &= x\,(1-x^2-y^2)(x^2+y^2-3) - y\,(2-x^2-y^2)\\
y' &= y\,(1-x^2-y^2)(x^2+ …
10
votes
Accepted
Riemannian metric adapted to singular $1$-dimensional foliation
No, this is not possible. In fact a more general result holds: If a vector field $X$ has an isolated singularity at $x\in M$ for which the linearization $X'(x):T_xM\to T_xM$ has no real eigenvalues, …
8
votes
Accepted
Non conformally geodesible vector field
Here is how one can construct an example: Consider the smooth, nonvanishing $1$-form
$$
\omega = y^3(1{-}y)^2\,\mathrm{d}x + \big(y^3-2(1{-}y)^2\bigr)\,\mathrm{d}y.
$$
Note: This $\omega$ came from …
8
votes
Accepted
An explicit formula for a flat metric compatible to certain polynomial vector field with center
Since the metric doesn't have to extend to the origin, take the flat metric
$$
g = \frac{\bigl(\mathrm{d}\left(x\sqrt{1+x^2/2}\right)\bigr)^2 + \mathrm{d}y^2}{x^2+x^4/2+y^2}.
$$
The level curves $x^2+ …
48
votes
Accepted
Finding a 1-form adapted to a smooth flow
If I understand correctly, there is already a counterexample on the torus:
On the $xy$-plane $\mathbb{R}^2$, let $X$ be the vector field
$$
X = \sin x\,\frac{\partial\ }{\partial x} + \cos x\,\frac{\ …
2
votes
Accepted
Transformation which sends asymptotic lines to principal lines over a surface
I don't know a reference, but, as you've stated it, this is a trivial result:
If $p$ is a point on a smooth surface $S\subset\mathbb{R}^3$ at which the Gauss curvature is negative, then $p$ is non- …
13
votes
Vector field with holomorphic flow
As Ben's argument suggests, the proof that, if the flow of $X$ preserves $J$ then the flow of $JX$ preserves $J$ does depend on the integrability of $J$.
As a concrete example of an almost-complex ma …
2
votes
Accepted
A cohomology associated with a codimension one foliation
First, it's not finite dimensional, even in the case of a torus. Just let $x,y$ be the $2\pi$-periodic functions on the torus and take $\alpha = \mathrm{d} x$, and you'll see that $H^0$ is all the fun …