Are the singular points of harmonic function on the disk always of measure zero?
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Let $f : mathbb D^2 to mathbb R$ be a smooth function with no singular points, i.e. $df neq 0$ on $mathbb D^2$. (Here $mathbb D^2$ is the closed unit disk in $mathbb R^2$).
Let $omega:mathbb D^2 to mathbb R$ be the harmonic function corresponding to the Dirichlet problem imposed by $f$, i.e $omega|_{partial mathbb D^2}=f|_{partial mathbb D^2}$.
Is it true that $domega neq 0$ on a set of full measure in $M$?
*By harmonic I mean $Delta omega=omega_{xx}+omega_{yy}=0$.
differential-topology riemannian-geometry harmonic-functions singularity
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add a comment |
$begingroup$
Let $f : mathbb D^2 to mathbb R$ be a smooth function with no singular points, i.e. $df neq 0$ on $mathbb D^2$. (Here $mathbb D^2$ is the closed unit disk in $mathbb R^2$).
Let $omega:mathbb D^2 to mathbb R$ be the harmonic function corresponding to the Dirichlet problem imposed by $f$, i.e $omega|_{partial mathbb D^2}=f|_{partial mathbb D^2}$.
Is it true that $domega neq 0$ on a set of full measure in $M$?
*By harmonic I mean $Delta omega=omega_{xx}+omega_{yy}=0$.
differential-topology riemannian-geometry harmonic-functions singularity
$endgroup$
add a comment |
$begingroup$
Let $f : mathbb D^2 to mathbb R$ be a smooth function with no singular points, i.e. $df neq 0$ on $mathbb D^2$. (Here $mathbb D^2$ is the closed unit disk in $mathbb R^2$).
Let $omega:mathbb D^2 to mathbb R$ be the harmonic function corresponding to the Dirichlet problem imposed by $f$, i.e $omega|_{partial mathbb D^2}=f|_{partial mathbb D^2}$.
Is it true that $domega neq 0$ on a set of full measure in $M$?
*By harmonic I mean $Delta omega=omega_{xx}+omega_{yy}=0$.
differential-topology riemannian-geometry harmonic-functions singularity
$endgroup$
Let $f : mathbb D^2 to mathbb R$ be a smooth function with no singular points, i.e. $df neq 0$ on $mathbb D^2$. (Here $mathbb D^2$ is the closed unit disk in $mathbb R^2$).
Let $omega:mathbb D^2 to mathbb R$ be the harmonic function corresponding to the Dirichlet problem imposed by $f$, i.e $omega|_{partial mathbb D^2}=f|_{partial mathbb D^2}$.
Is it true that $domega neq 0$ on a set of full measure in $M$?
*By harmonic I mean $Delta omega=omega_{xx}+omega_{yy}=0$.
differential-topology riemannian-geometry harmonic-functions singularity
differential-topology riemannian-geometry harmonic-functions singularity
asked Jan 7 at 13:17
Asaf ShacharAsaf Shachar
5,79931145
5,79931145
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After speaking with a colleague, here is a possible solution:
Sine $omega$ is harmonic, it is real-analytic. In particular its partial derivatives $omega_x,omega_y:mathbb D^2 to mathbb R$ are real-analytic. Define $A={ pin mathbb D^2 , | , omega_x(p)=omega_y(p)=0}$. We shall prove $A$ has measure zero. Indeed, $A$ is closed. So, if it had positive measure, then it would contain an accumulation point in $operatorname{Int} mathbb D^2$ (see the lemma below). By the identity theorem, this would imply $omega_x=omega_y=0$ on $operatorname{Int} mathbb D^2$, which would imply $omega$ is constant on $mathbb D^2$. However, $f$ cannot be constant* on $partial mathbb D^2$ which is a contradiction to $f|_{partial mathbb D^2}=omega|_{partial mathbb D^2}$.
$f$ is not constant on $partial mathbb D^2$: Indeed, we assumed that $df neq 0$ everywhere, so $min f,max f$ are both obtained on $partial mathbb D^2$, and are distinct, since $f$ is not constant on the whole disk.
Lemma: A closed subset $A subseteq mathbb D^2$ of positive measure contains an accumulation point in $operatorname{Int} mathbb D^2$.
Proof:
Assume by contradiction that $A$ does not contain an accumulation point in $operatorname{Int} mathbb D^2$. This implies (by compactness), that for any natural $n$, $A cap B_{1-1/n}$ is finite, where $B_r$ is the closed disk of radius $r$. Thus, $A cap operatorname{Int} mathbb D^2=cup_n A cap B_{1-1/n}$ is countable, hence of measure zero. Thus $A$ has measure zero, contradiction.
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1 Answer
1
active
oldest
votes
1 Answer
1
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
After speaking with a colleague, here is a possible solution:
Sine $omega$ is harmonic, it is real-analytic. In particular its partial derivatives $omega_x,omega_y:mathbb D^2 to mathbb R$ are real-analytic. Define $A={ pin mathbb D^2 , | , omega_x(p)=omega_y(p)=0}$. We shall prove $A$ has measure zero. Indeed, $A$ is closed. So, if it had positive measure, then it would contain an accumulation point in $operatorname{Int} mathbb D^2$ (see the lemma below). By the identity theorem, this would imply $omega_x=omega_y=0$ on $operatorname{Int} mathbb D^2$, which would imply $omega$ is constant on $mathbb D^2$. However, $f$ cannot be constant* on $partial mathbb D^2$ which is a contradiction to $f|_{partial mathbb D^2}=omega|_{partial mathbb D^2}$.
$f$ is not constant on $partial mathbb D^2$: Indeed, we assumed that $df neq 0$ everywhere, so $min f,max f$ are both obtained on $partial mathbb D^2$, and are distinct, since $f$ is not constant on the whole disk.
Lemma: A closed subset $A subseteq mathbb D^2$ of positive measure contains an accumulation point in $operatorname{Int} mathbb D^2$.
Proof:
Assume by contradiction that $A$ does not contain an accumulation point in $operatorname{Int} mathbb D^2$. This implies (by compactness), that for any natural $n$, $A cap B_{1-1/n}$ is finite, where $B_r$ is the closed disk of radius $r$. Thus, $A cap operatorname{Int} mathbb D^2=cup_n A cap B_{1-1/n}$ is countable, hence of measure zero. Thus $A$ has measure zero, contradiction.
$endgroup$
add a comment |
$begingroup$
After speaking with a colleague, here is a possible solution:
Sine $omega$ is harmonic, it is real-analytic. In particular its partial derivatives $omega_x,omega_y:mathbb D^2 to mathbb R$ are real-analytic. Define $A={ pin mathbb D^2 , | , omega_x(p)=omega_y(p)=0}$. We shall prove $A$ has measure zero. Indeed, $A$ is closed. So, if it had positive measure, then it would contain an accumulation point in $operatorname{Int} mathbb D^2$ (see the lemma below). By the identity theorem, this would imply $omega_x=omega_y=0$ on $operatorname{Int} mathbb D^2$, which would imply $omega$ is constant on $mathbb D^2$. However, $f$ cannot be constant* on $partial mathbb D^2$ which is a contradiction to $f|_{partial mathbb D^2}=omega|_{partial mathbb D^2}$.
$f$ is not constant on $partial mathbb D^2$: Indeed, we assumed that $df neq 0$ everywhere, so $min f,max f$ are both obtained on $partial mathbb D^2$, and are distinct, since $f$ is not constant on the whole disk.
Lemma: A closed subset $A subseteq mathbb D^2$ of positive measure contains an accumulation point in $operatorname{Int} mathbb D^2$.
Proof:
Assume by contradiction that $A$ does not contain an accumulation point in $operatorname{Int} mathbb D^2$. This implies (by compactness), that for any natural $n$, $A cap B_{1-1/n}$ is finite, where $B_r$ is the closed disk of radius $r$. Thus, $A cap operatorname{Int} mathbb D^2=cup_n A cap B_{1-1/n}$ is countable, hence of measure zero. Thus $A$ has measure zero, contradiction.
$endgroup$
add a comment |
$begingroup$
After speaking with a colleague, here is a possible solution:
Sine $omega$ is harmonic, it is real-analytic. In particular its partial derivatives $omega_x,omega_y:mathbb D^2 to mathbb R$ are real-analytic. Define $A={ pin mathbb D^2 , | , omega_x(p)=omega_y(p)=0}$. We shall prove $A$ has measure zero. Indeed, $A$ is closed. So, if it had positive measure, then it would contain an accumulation point in $operatorname{Int} mathbb D^2$ (see the lemma below). By the identity theorem, this would imply $omega_x=omega_y=0$ on $operatorname{Int} mathbb D^2$, which would imply $omega$ is constant on $mathbb D^2$. However, $f$ cannot be constant* on $partial mathbb D^2$ which is a contradiction to $f|_{partial mathbb D^2}=omega|_{partial mathbb D^2}$.
$f$ is not constant on $partial mathbb D^2$: Indeed, we assumed that $df neq 0$ everywhere, so $min f,max f$ are both obtained on $partial mathbb D^2$, and are distinct, since $f$ is not constant on the whole disk.
Lemma: A closed subset $A subseteq mathbb D^2$ of positive measure contains an accumulation point in $operatorname{Int} mathbb D^2$.
Proof:
Assume by contradiction that $A$ does not contain an accumulation point in $operatorname{Int} mathbb D^2$. This implies (by compactness), that for any natural $n$, $A cap B_{1-1/n}$ is finite, where $B_r$ is the closed disk of radius $r$. Thus, $A cap operatorname{Int} mathbb D^2=cup_n A cap B_{1-1/n}$ is countable, hence of measure zero. Thus $A$ has measure zero, contradiction.
$endgroup$
After speaking with a colleague, here is a possible solution:
Sine $omega$ is harmonic, it is real-analytic. In particular its partial derivatives $omega_x,omega_y:mathbb D^2 to mathbb R$ are real-analytic. Define $A={ pin mathbb D^2 , | , omega_x(p)=omega_y(p)=0}$. We shall prove $A$ has measure zero. Indeed, $A$ is closed. So, if it had positive measure, then it would contain an accumulation point in $operatorname{Int} mathbb D^2$ (see the lemma below). By the identity theorem, this would imply $omega_x=omega_y=0$ on $operatorname{Int} mathbb D^2$, which would imply $omega$ is constant on $mathbb D^2$. However, $f$ cannot be constant* on $partial mathbb D^2$ which is a contradiction to $f|_{partial mathbb D^2}=omega|_{partial mathbb D^2}$.
$f$ is not constant on $partial mathbb D^2$: Indeed, we assumed that $df neq 0$ everywhere, so $min f,max f$ are both obtained on $partial mathbb D^2$, and are distinct, since $f$ is not constant on the whole disk.
Lemma: A closed subset $A subseteq mathbb D^2$ of positive measure contains an accumulation point in $operatorname{Int} mathbb D^2$.
Proof:
Assume by contradiction that $A$ does not contain an accumulation point in $operatorname{Int} mathbb D^2$. This implies (by compactness), that for any natural $n$, $A cap B_{1-1/n}$ is finite, where $B_r$ is the closed disk of radius $r$. Thus, $A cap operatorname{Int} mathbb D^2=cup_n A cap B_{1-1/n}$ is countable, hence of measure zero. Thus $A$ has measure zero, contradiction.
answered Jan 7 at 14:36
Asaf ShacharAsaf Shachar
5,79931145
5,79931145
add a comment |
add a comment |
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