Can this Helmholtz PDE with Robin boundary conditions be solved analytically?












2












$begingroup$


Consider the following Helmholtz problem in the infinite triangle $y>0,;x>y$ with parameters $Q<0$, $Pge0$, $P<|Q|$.



$$left{begin{align}
&psi^{(2,0)}(x,y)+psi^{(0,2)}(x,y)+Epsi(x,y)=0,\
&psi^{(0,1)}(x,0)-frac Q2psi(x,0)=0,\
&psi^{(1,0)}(x,x)-psi^{(0,1)}(x,x)-frac P{sqrt2}psi(x,x)=0\
&|psi(x,y)|<infty.
end{align}right.tag1
$$



I'm mainly interested in the solution with lowest $E$. In the case of $P=0$ it's easy to see that



$$psi_0(x,y)=expleft(frac Q2 (x+y)right)tag2$$



with eigenvalue



$$E=-frac{Q^2}2tag3$$



solves the problem. But what about $P>0$? Can $(1)$ still be solved analytically (i.e. in terms of elementary or special functions)? If not, can the solution be given in the form of an integral or a series with explicitly specified terms?










share|cite|improve this question









$endgroup$

















    2












    $begingroup$


    Consider the following Helmholtz problem in the infinite triangle $y>0,;x>y$ with parameters $Q<0$, $Pge0$, $P<|Q|$.



    $$left{begin{align}
    &psi^{(2,0)}(x,y)+psi^{(0,2)}(x,y)+Epsi(x,y)=0,\
    &psi^{(0,1)}(x,0)-frac Q2psi(x,0)=0,\
    &psi^{(1,0)}(x,x)-psi^{(0,1)}(x,x)-frac P{sqrt2}psi(x,x)=0\
    &|psi(x,y)|<infty.
    end{align}right.tag1
    $$



    I'm mainly interested in the solution with lowest $E$. In the case of $P=0$ it's easy to see that



    $$psi_0(x,y)=expleft(frac Q2 (x+y)right)tag2$$



    with eigenvalue



    $$E=-frac{Q^2}2tag3$$



    solves the problem. But what about $P>0$? Can $(1)$ still be solved analytically (i.e. in terms of elementary or special functions)? If not, can the solution be given in the form of an integral or a series with explicitly specified terms?










    share|cite|improve this question









    $endgroup$















      2












      2








      2


      2



      $begingroup$


      Consider the following Helmholtz problem in the infinite triangle $y>0,;x>y$ with parameters $Q<0$, $Pge0$, $P<|Q|$.



      $$left{begin{align}
      &psi^{(2,0)}(x,y)+psi^{(0,2)}(x,y)+Epsi(x,y)=0,\
      &psi^{(0,1)}(x,0)-frac Q2psi(x,0)=0,\
      &psi^{(1,0)}(x,x)-psi^{(0,1)}(x,x)-frac P{sqrt2}psi(x,x)=0\
      &|psi(x,y)|<infty.
      end{align}right.tag1
      $$



      I'm mainly interested in the solution with lowest $E$. In the case of $P=0$ it's easy to see that



      $$psi_0(x,y)=expleft(frac Q2 (x+y)right)tag2$$



      with eigenvalue



      $$E=-frac{Q^2}2tag3$$



      solves the problem. But what about $P>0$? Can $(1)$ still be solved analytically (i.e. in terms of elementary or special functions)? If not, can the solution be given in the form of an integral or a series with explicitly specified terms?










      share|cite|improve this question









      $endgroup$




      Consider the following Helmholtz problem in the infinite triangle $y>0,;x>y$ with parameters $Q<0$, $Pge0$, $P<|Q|$.



      $$left{begin{align}
      &psi^{(2,0)}(x,y)+psi^{(0,2)}(x,y)+Epsi(x,y)=0,\
      &psi^{(0,1)}(x,0)-frac Q2psi(x,0)=0,\
      &psi^{(1,0)}(x,x)-psi^{(0,1)}(x,x)-frac P{sqrt2}psi(x,x)=0\
      &|psi(x,y)|<infty.
      end{align}right.tag1
      $$



      I'm mainly interested in the solution with lowest $E$. In the case of $P=0$ it's easy to see that



      $$psi_0(x,y)=expleft(frac Q2 (x+y)right)tag2$$



      with eigenvalue



      $$E=-frac{Q^2}2tag3$$



      solves the problem. But what about $P>0$? Can $(1)$ still be solved analytically (i.e. in terms of elementary or special functions)? If not, can the solution be given in the form of an integral or a series with explicitly specified terms?







      pde closed-form boundary-value-problem eigenfunctions






      share|cite|improve this question













      share|cite|improve this question











      share|cite|improve this question




      share|cite|improve this question










      asked Jan 7 at 10:18









      RuslanRuslan

      3,72721533




      3,72721533






















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