Asymptotic solution












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I am looking for asymptotic solutions to the equation
$$alpha^{-1}x+sqrt{pi}frac{sqrt{x}}{2}text{erf}left(frac{sqrt{x}}{2}right)=beta^{-1}e^{-x/4},qquad alphall1,betagg1.$$ When $alpha$ is large and the first term is negligible, this is easy to do, but I don't know how to proceed with the opposite case.



What I've tried for now is the following: For $alpha,beta^{-1}=0$, which is the limiting case, I get $x=0$, hence I have to introduce a scaling $x=epsilonhat x$, where $epsilon=epsilon(alpha,beta)ll1$. Introducing this into the equation above allows me to simplify terms and reduce the equation (if I'm not wrong) to
$$epsilon(1color{red}{+}alpha/2)hat x=alphabeta^{-1},$$ therefore I can balance the equation by choosing $epsilon=alphabeta^{-1}$ and finally $$hat xapproxcolor{red}{2/(2+alpha)}qquadRightarrowqquad xapproxalphabeta^{-1}.$$



Is this correct? Any hints or help on this?



Thanks in advance!



$color{red}{text{Edit: The leading order term had a mistake, I have corrected it.}}$










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    1












    $begingroup$


    I am looking for asymptotic solutions to the equation
    $$alpha^{-1}x+sqrt{pi}frac{sqrt{x}}{2}text{erf}left(frac{sqrt{x}}{2}right)=beta^{-1}e^{-x/4},qquad alphall1,betagg1.$$ When $alpha$ is large and the first term is negligible, this is easy to do, but I don't know how to proceed with the opposite case.



    What I've tried for now is the following: For $alpha,beta^{-1}=0$, which is the limiting case, I get $x=0$, hence I have to introduce a scaling $x=epsilonhat x$, where $epsilon=epsilon(alpha,beta)ll1$. Introducing this into the equation above allows me to simplify terms and reduce the equation (if I'm not wrong) to
    $$epsilon(1color{red}{+}alpha/2)hat x=alphabeta^{-1},$$ therefore I can balance the equation by choosing $epsilon=alphabeta^{-1}$ and finally $$hat xapproxcolor{red}{2/(2+alpha)}qquadRightarrowqquad xapproxalphabeta^{-1}.$$



    Is this correct? Any hints or help on this?



    Thanks in advance!



    $color{red}{text{Edit: The leading order term had a mistake, I have corrected it.}}$










    share|cite|improve this question











    $endgroup$















      1












      1








      1





      $begingroup$


      I am looking for asymptotic solutions to the equation
      $$alpha^{-1}x+sqrt{pi}frac{sqrt{x}}{2}text{erf}left(frac{sqrt{x}}{2}right)=beta^{-1}e^{-x/4},qquad alphall1,betagg1.$$ When $alpha$ is large and the first term is negligible, this is easy to do, but I don't know how to proceed with the opposite case.



      What I've tried for now is the following: For $alpha,beta^{-1}=0$, which is the limiting case, I get $x=0$, hence I have to introduce a scaling $x=epsilonhat x$, where $epsilon=epsilon(alpha,beta)ll1$. Introducing this into the equation above allows me to simplify terms and reduce the equation (if I'm not wrong) to
      $$epsilon(1color{red}{+}alpha/2)hat x=alphabeta^{-1},$$ therefore I can balance the equation by choosing $epsilon=alphabeta^{-1}$ and finally $$hat xapproxcolor{red}{2/(2+alpha)}qquadRightarrowqquad xapproxalphabeta^{-1}.$$



      Is this correct? Any hints or help on this?



      Thanks in advance!



      $color{red}{text{Edit: The leading order term had a mistake, I have corrected it.}}$










      share|cite|improve this question











      $endgroup$




      I am looking for asymptotic solutions to the equation
      $$alpha^{-1}x+sqrt{pi}frac{sqrt{x}}{2}text{erf}left(frac{sqrt{x}}{2}right)=beta^{-1}e^{-x/4},qquad alphall1,betagg1.$$ When $alpha$ is large and the first term is negligible, this is easy to do, but I don't know how to proceed with the opposite case.



      What I've tried for now is the following: For $alpha,beta^{-1}=0$, which is the limiting case, I get $x=0$, hence I have to introduce a scaling $x=epsilonhat x$, where $epsilon=epsilon(alpha,beta)ll1$. Introducing this into the equation above allows me to simplify terms and reduce the equation (if I'm not wrong) to
      $$epsilon(1color{red}{+}alpha/2)hat x=alphabeta^{-1},$$ therefore I can balance the equation by choosing $epsilon=alphabeta^{-1}$ and finally $$hat xapproxcolor{red}{2/(2+alpha)}qquadRightarrowqquad xapproxalphabeta^{-1}.$$



      Is this correct? Any hints or help on this?



      Thanks in advance!



      $color{red}{text{Edit: The leading order term had a mistake, I have corrected it.}}$







      asymptotics






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      edited Feb 1 at 10:34







      Marc

















      asked Dec 21 '18 at 10:20









      MarcMarc

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      44139






















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          $begingroup$

          Let $tilde beta = 1/beta$. Multiplying by $alpha$ and getting rid of the square roots, we can rewrite the equation as
          $$x - alpha tilde beta e^{-x/4} +
          alpha x int_0^{1/2} e^{-x t^2} d t = 0.$$

          Now we can look for $x$ in the form $sum c_{i,j} alpha^i tilde beta {}^j$ by substituting the sum into the equation and taking the bivariate Taylor expansion around $alpha = 0, ,tilde beta = 0$.



          Taking $x = alpha tilde beta + sum_{i = 0}^3 c_{i, 3 - i} alpha^i tilde beta {}^{3 - i}$ gives
          $$c_{3, 0} alpha^3 +
          left( c_{2, 1} + frac 1 2 right) alpha^2 tilde beta +
          c_{1, 2} alpha tilde beta {}^2 +
          c_{0, 3} tilde beta {}^3 = 0,$$

          therefore we get one third-order term $-alpha^2 tilde beta/2$.



          On the next step we get two fourth-order terms, which gives the approximation
          $$x approx frac alpha beta -frac {alpha^2} {2 beta} +
          frac {alpha^3} {4 beta} - frac {alpha^2} {4 beta^2}.$$






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            $begingroup$

            Let $tilde beta = 1/beta$. Multiplying by $alpha$ and getting rid of the square roots, we can rewrite the equation as
            $$x - alpha tilde beta e^{-x/4} +
            alpha x int_0^{1/2} e^{-x t^2} d t = 0.$$

            Now we can look for $x$ in the form $sum c_{i,j} alpha^i tilde beta {}^j$ by substituting the sum into the equation and taking the bivariate Taylor expansion around $alpha = 0, ,tilde beta = 0$.



            Taking $x = alpha tilde beta + sum_{i = 0}^3 c_{i, 3 - i} alpha^i tilde beta {}^{3 - i}$ gives
            $$c_{3, 0} alpha^3 +
            left( c_{2, 1} + frac 1 2 right) alpha^2 tilde beta +
            c_{1, 2} alpha tilde beta {}^2 +
            c_{0, 3} tilde beta {}^3 = 0,$$

            therefore we get one third-order term $-alpha^2 tilde beta/2$.



            On the next step we get two fourth-order terms, which gives the approximation
            $$x approx frac alpha beta -frac {alpha^2} {2 beta} +
            frac {alpha^3} {4 beta} - frac {alpha^2} {4 beta^2}.$$






            share|cite|improve this answer











            $endgroup$


















              0












              $begingroup$

              Let $tilde beta = 1/beta$. Multiplying by $alpha$ and getting rid of the square roots, we can rewrite the equation as
              $$x - alpha tilde beta e^{-x/4} +
              alpha x int_0^{1/2} e^{-x t^2} d t = 0.$$

              Now we can look for $x$ in the form $sum c_{i,j} alpha^i tilde beta {}^j$ by substituting the sum into the equation and taking the bivariate Taylor expansion around $alpha = 0, ,tilde beta = 0$.



              Taking $x = alpha tilde beta + sum_{i = 0}^3 c_{i, 3 - i} alpha^i tilde beta {}^{3 - i}$ gives
              $$c_{3, 0} alpha^3 +
              left( c_{2, 1} + frac 1 2 right) alpha^2 tilde beta +
              c_{1, 2} alpha tilde beta {}^2 +
              c_{0, 3} tilde beta {}^3 = 0,$$

              therefore we get one third-order term $-alpha^2 tilde beta/2$.



              On the next step we get two fourth-order terms, which gives the approximation
              $$x approx frac alpha beta -frac {alpha^2} {2 beta} +
              frac {alpha^3} {4 beta} - frac {alpha^2} {4 beta^2}.$$






              share|cite|improve this answer











              $endgroup$
















                0












                0








                0





                $begingroup$

                Let $tilde beta = 1/beta$. Multiplying by $alpha$ and getting rid of the square roots, we can rewrite the equation as
                $$x - alpha tilde beta e^{-x/4} +
                alpha x int_0^{1/2} e^{-x t^2} d t = 0.$$

                Now we can look for $x$ in the form $sum c_{i,j} alpha^i tilde beta {}^j$ by substituting the sum into the equation and taking the bivariate Taylor expansion around $alpha = 0, ,tilde beta = 0$.



                Taking $x = alpha tilde beta + sum_{i = 0}^3 c_{i, 3 - i} alpha^i tilde beta {}^{3 - i}$ gives
                $$c_{3, 0} alpha^3 +
                left( c_{2, 1} + frac 1 2 right) alpha^2 tilde beta +
                c_{1, 2} alpha tilde beta {}^2 +
                c_{0, 3} tilde beta {}^3 = 0,$$

                therefore we get one third-order term $-alpha^2 tilde beta/2$.



                On the next step we get two fourth-order terms, which gives the approximation
                $$x approx frac alpha beta -frac {alpha^2} {2 beta} +
                frac {alpha^3} {4 beta} - frac {alpha^2} {4 beta^2}.$$






                share|cite|improve this answer











                $endgroup$



                Let $tilde beta = 1/beta$. Multiplying by $alpha$ and getting rid of the square roots, we can rewrite the equation as
                $$x - alpha tilde beta e^{-x/4} +
                alpha x int_0^{1/2} e^{-x t^2} d t = 0.$$

                Now we can look for $x$ in the form $sum c_{i,j} alpha^i tilde beta {}^j$ by substituting the sum into the equation and taking the bivariate Taylor expansion around $alpha = 0, ,tilde beta = 0$.



                Taking $x = alpha tilde beta + sum_{i = 0}^3 c_{i, 3 - i} alpha^i tilde beta {}^{3 - i}$ gives
                $$c_{3, 0} alpha^3 +
                left( c_{2, 1} + frac 1 2 right) alpha^2 tilde beta +
                c_{1, 2} alpha tilde beta {}^2 +
                c_{0, 3} tilde beta {}^3 = 0,$$

                therefore we get one third-order term $-alpha^2 tilde beta/2$.



                On the next step we get two fourth-order terms, which gives the approximation
                $$x approx frac alpha beta -frac {alpha^2} {2 beta} +
                frac {alpha^3} {4 beta} - frac {alpha^2} {4 beta^2}.$$







                share|cite|improve this answer














                share|cite|improve this answer



                share|cite|improve this answer








                edited Jan 6 at 22:35

























                answered Dec 27 '18 at 22:12









                MaximMaxim

                6,2731221




                6,2731221






























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