Smooth vector fields on a surface modulo diffeomorphisms
$begingroup$
Let $Sigma$ be a two-dimensional connected smooth manifold without boundary. (Feel free to assume it is compact and orientable.)
Let $mathcal{X}(Sigma)$ denote the smooth vector fields on $Sigma$ and let $operatorname{Diff}(Sigma)$ denote the group of diffeomorphisms of $Sigma$. Clearly $operatorname{Diff}(Sigma)$ acts on $mathcal{X}(Sigma)$.
I would expect naively that the space of orbits $mathcal{M}:=mathcal{X}(Sigma)/operatorname{Diff}(Sigma)$ would be finite-dimensional. Is this actually the case?
Question
What can one say about $mathcal{M}$ in general?
Any references where I could read about this question would be appreciated.
dg.differential-geometry differential-topology smooth-manifolds infinite-dimensional-manifolds
$endgroup$
add a comment |
$begingroup$
Let $Sigma$ be a two-dimensional connected smooth manifold without boundary. (Feel free to assume it is compact and orientable.)
Let $mathcal{X}(Sigma)$ denote the smooth vector fields on $Sigma$ and let $operatorname{Diff}(Sigma)$ denote the group of diffeomorphisms of $Sigma$. Clearly $operatorname{Diff}(Sigma)$ acts on $mathcal{X}(Sigma)$.
I would expect naively that the space of orbits $mathcal{M}:=mathcal{X}(Sigma)/operatorname{Diff}(Sigma)$ would be finite-dimensional. Is this actually the case?
Question
What can one say about $mathcal{M}$ in general?
Any references where I could read about this question would be appreciated.
dg.differential-geometry differential-topology smooth-manifolds infinite-dimensional-manifolds
$endgroup$
add a comment |
$begingroup$
Let $Sigma$ be a two-dimensional connected smooth manifold without boundary. (Feel free to assume it is compact and orientable.)
Let $mathcal{X}(Sigma)$ denote the smooth vector fields on $Sigma$ and let $operatorname{Diff}(Sigma)$ denote the group of diffeomorphisms of $Sigma$. Clearly $operatorname{Diff}(Sigma)$ acts on $mathcal{X}(Sigma)$.
I would expect naively that the space of orbits $mathcal{M}:=mathcal{X}(Sigma)/operatorname{Diff}(Sigma)$ would be finite-dimensional. Is this actually the case?
Question
What can one say about $mathcal{M}$ in general?
Any references where I could read about this question would be appreciated.
dg.differential-geometry differential-topology smooth-manifolds infinite-dimensional-manifolds
$endgroup$
Let $Sigma$ be a two-dimensional connected smooth manifold without boundary. (Feel free to assume it is compact and orientable.)
Let $mathcal{X}(Sigma)$ denote the smooth vector fields on $Sigma$ and let $operatorname{Diff}(Sigma)$ denote the group of diffeomorphisms of $Sigma$. Clearly $operatorname{Diff}(Sigma)$ acts on $mathcal{X}(Sigma)$.
I would expect naively that the space of orbits $mathcal{M}:=mathcal{X}(Sigma)/operatorname{Diff}(Sigma)$ would be finite-dimensional. Is this actually the case?
Question
What can one say about $mathcal{M}$ in general?
Any references where I could read about this question would be appreciated.
dg.differential-geometry differential-topology smooth-manifolds infinite-dimensional-manifolds
dg.differential-geometry differential-topology smooth-manifolds infinite-dimensional-manifolds
edited 12 hours ago
YCor
28.2k483136
28.2k483136
asked 12 hours ago
José Figueroa-O'FarrillJosé Figueroa-O'Farrill
25.5k373150
25.5k373150
add a comment |
add a comment |
1 Answer
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$begingroup$
This is not finite dimensional. For example, consider non-vanishing vector fields on $T^2=mathbb R^2/mathbb Z^2$, transversal to vertical circles. Any such field defines a self diffeo $S^1to S^1$ on a vertical circle, called the return map. Suppose that such a diffeo $varphi$ has $n$ fixed points $x_i$ (they correspond to closed orbits of the field). Then for each fixed point $x_iin S^1$ we have a linear map on the tangent space $dvarphi: T_{x_i}S^1to T_{x_i}S^1$ given by multiplication by $alpha_iin mathbb R^*$. Such $alpha_i$ is an invariant of a vector field under diffeomorphisms. And since the number of closed orbits can be arbitrary and these $alpha_i$'s are independent, we see that the dimension is not finite.
If you want something which is finite-dimensional, one can restrict to area-preserving vector fields which are same thing as closed $1$-forms. Now the spaces of minimal closed $1$-forms on a closed genus $g$ surface is indeed finite-dimensional by a theorem of Calabi. Each such form is the real part of a holomorphic $1$-form for a certain complex structure on the surface. (the reference is: E. Calabi, An intrinsic characterization of harmonic 1-forms, Global Analysis, Papers in Honor of K. Kodaira, 1969)
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$begingroup$
This is not finite dimensional. For example, consider non-vanishing vector fields on $T^2=mathbb R^2/mathbb Z^2$, transversal to vertical circles. Any such field defines a self diffeo $S^1to S^1$ on a vertical circle, called the return map. Suppose that such a diffeo $varphi$ has $n$ fixed points $x_i$ (they correspond to closed orbits of the field). Then for each fixed point $x_iin S^1$ we have a linear map on the tangent space $dvarphi: T_{x_i}S^1to T_{x_i}S^1$ given by multiplication by $alpha_iin mathbb R^*$. Such $alpha_i$ is an invariant of a vector field under diffeomorphisms. And since the number of closed orbits can be arbitrary and these $alpha_i$'s are independent, we see that the dimension is not finite.
If you want something which is finite-dimensional, one can restrict to area-preserving vector fields which are same thing as closed $1$-forms. Now the spaces of minimal closed $1$-forms on a closed genus $g$ surface is indeed finite-dimensional by a theorem of Calabi. Each such form is the real part of a holomorphic $1$-form for a certain complex structure on the surface. (the reference is: E. Calabi, An intrinsic characterization of harmonic 1-forms, Global Analysis, Papers in Honor of K. Kodaira, 1969)
$endgroup$
add a comment |
$begingroup$
This is not finite dimensional. For example, consider non-vanishing vector fields on $T^2=mathbb R^2/mathbb Z^2$, transversal to vertical circles. Any such field defines a self diffeo $S^1to S^1$ on a vertical circle, called the return map. Suppose that such a diffeo $varphi$ has $n$ fixed points $x_i$ (they correspond to closed orbits of the field). Then for each fixed point $x_iin S^1$ we have a linear map on the tangent space $dvarphi: T_{x_i}S^1to T_{x_i}S^1$ given by multiplication by $alpha_iin mathbb R^*$. Such $alpha_i$ is an invariant of a vector field under diffeomorphisms. And since the number of closed orbits can be arbitrary and these $alpha_i$'s are independent, we see that the dimension is not finite.
If you want something which is finite-dimensional, one can restrict to area-preserving vector fields which are same thing as closed $1$-forms. Now the spaces of minimal closed $1$-forms on a closed genus $g$ surface is indeed finite-dimensional by a theorem of Calabi. Each such form is the real part of a holomorphic $1$-form for a certain complex structure on the surface. (the reference is: E. Calabi, An intrinsic characterization of harmonic 1-forms, Global Analysis, Papers in Honor of K. Kodaira, 1969)
$endgroup$
add a comment |
$begingroup$
This is not finite dimensional. For example, consider non-vanishing vector fields on $T^2=mathbb R^2/mathbb Z^2$, transversal to vertical circles. Any such field defines a self diffeo $S^1to S^1$ on a vertical circle, called the return map. Suppose that such a diffeo $varphi$ has $n$ fixed points $x_i$ (they correspond to closed orbits of the field). Then for each fixed point $x_iin S^1$ we have a linear map on the tangent space $dvarphi: T_{x_i}S^1to T_{x_i}S^1$ given by multiplication by $alpha_iin mathbb R^*$. Such $alpha_i$ is an invariant of a vector field under diffeomorphisms. And since the number of closed orbits can be arbitrary and these $alpha_i$'s are independent, we see that the dimension is not finite.
If you want something which is finite-dimensional, one can restrict to area-preserving vector fields which are same thing as closed $1$-forms. Now the spaces of minimal closed $1$-forms on a closed genus $g$ surface is indeed finite-dimensional by a theorem of Calabi. Each such form is the real part of a holomorphic $1$-form for a certain complex structure on the surface. (the reference is: E. Calabi, An intrinsic characterization of harmonic 1-forms, Global Analysis, Papers in Honor of K. Kodaira, 1969)
$endgroup$
This is not finite dimensional. For example, consider non-vanishing vector fields on $T^2=mathbb R^2/mathbb Z^2$, transversal to vertical circles. Any such field defines a self diffeo $S^1to S^1$ on a vertical circle, called the return map. Suppose that such a diffeo $varphi$ has $n$ fixed points $x_i$ (they correspond to closed orbits of the field). Then for each fixed point $x_iin S^1$ we have a linear map on the tangent space $dvarphi: T_{x_i}S^1to T_{x_i}S^1$ given by multiplication by $alpha_iin mathbb R^*$. Such $alpha_i$ is an invariant of a vector field under diffeomorphisms. And since the number of closed orbits can be arbitrary and these $alpha_i$'s are independent, we see that the dimension is not finite.
If you want something which is finite-dimensional, one can restrict to area-preserving vector fields which are same thing as closed $1$-forms. Now the spaces of minimal closed $1$-forms on a closed genus $g$ surface is indeed finite-dimensional by a theorem of Calabi. Each such form is the real part of a holomorphic $1$-form for a certain complex structure on the surface. (the reference is: E. Calabi, An intrinsic characterization of harmonic 1-forms, Global Analysis, Papers in Honor of K. Kodaira, 1969)
edited 11 hours ago
answered 11 hours ago
Dmitri PanovDmitri Panov
19.5k460121
19.5k460121
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