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 $Delta omega=omega_{xx}+omega_{yy}=0$.










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    1












    $begingroup$


    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 $Delta omega=omega_{xx}+omega_{yy}=0$.










    share|cite|improve this question









    $endgroup$















      1












      1








      1


      1



      $begingroup$


      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 $Delta omega=omega_{xx}+omega_{yy}=0$.










      share|cite|improve this question









      $endgroup$




      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






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      asked Jan 7 at 13:17









      Asaf ShacharAsaf Shachar

      5,79931145




      5,79931145






















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          $begingroup$

          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.






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            1 Answer
            1






            active

            oldest

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            1 Answer
            1






            active

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            votes









            active

            oldest

            votes






            active

            oldest

            votes









            1












            $begingroup$

            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.






            share|cite|improve this answer









            $endgroup$


















              1












              $begingroup$

              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.






              share|cite|improve this answer









              $endgroup$
















                1












                1








                1





                $begingroup$

                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.






                share|cite|improve this answer









                $endgroup$



                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.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Jan 7 at 14:36









                Asaf ShacharAsaf Shachar

                5,79931145




                5,79931145






























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