Sign of the derivative of the Hankel Function with purely imaginary arguments












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Consider the Hankel function of the first kind $H^{(1)}_nu (z)$.
If I restrict $z$ to be a purely imaginary number of the form $ix$ where $x in mathbb{R}$ and $x>0$ and let $nu =0$. We can see that $iH^{(1)}_0 (ix) > 0$. Using the standard recursion relationship for the derivatives of the Hankel (and Bessel) functions, we see that $frac{partial}{partial x} big(iH^{(1)}_0 (ix)big) = H^{(1)}_1 (ix)$, and running some calculations, we see that $H^{(1)} _1 (ix) < 0$ for $x>0$.



If you continue taking the $x$ derivatives of $iH_0 ^{(1)} (ix)$, the sign of the derivatives alternates for $x>0$. My question is, how do I prove that for even $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) >0$ and for odd $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) <0$?










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    Consider the Hankel function of the first kind $H^{(1)}_nu (z)$.
    If I restrict $z$ to be a purely imaginary number of the form $ix$ where $x in mathbb{R}$ and $x>0$ and let $nu =0$. We can see that $iH^{(1)}_0 (ix) > 0$. Using the standard recursion relationship for the derivatives of the Hankel (and Bessel) functions, we see that $frac{partial}{partial x} big(iH^{(1)}_0 (ix)big) = H^{(1)}_1 (ix)$, and running some calculations, we see that $H^{(1)} _1 (ix) < 0$ for $x>0$.



    If you continue taking the $x$ derivatives of $iH_0 ^{(1)} (ix)$, the sign of the derivatives alternates for $x>0$. My question is, how do I prove that for even $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) >0$ and for odd $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) <0$?










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      1







      Consider the Hankel function of the first kind $H^{(1)}_nu (z)$.
      If I restrict $z$ to be a purely imaginary number of the form $ix$ where $x in mathbb{R}$ and $x>0$ and let $nu =0$. We can see that $iH^{(1)}_0 (ix) > 0$. Using the standard recursion relationship for the derivatives of the Hankel (and Bessel) functions, we see that $frac{partial}{partial x} big(iH^{(1)}_0 (ix)big) = H^{(1)}_1 (ix)$, and running some calculations, we see that $H^{(1)} _1 (ix) < 0$ for $x>0$.



      If you continue taking the $x$ derivatives of $iH_0 ^{(1)} (ix)$, the sign of the derivatives alternates for $x>0$. My question is, how do I prove that for even $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) >0$ and for odd $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) <0$?










      share|cite|improve this question













      Consider the Hankel function of the first kind $H^{(1)}_nu (z)$.
      If I restrict $z$ to be a purely imaginary number of the form $ix$ where $x in mathbb{R}$ and $x>0$ and let $nu =0$. We can see that $iH^{(1)}_0 (ix) > 0$. Using the standard recursion relationship for the derivatives of the Hankel (and Bessel) functions, we see that $frac{partial}{partial x} big(iH^{(1)}_0 (ix)big) = H^{(1)}_1 (ix)$, and running some calculations, we see that $H^{(1)} _1 (ix) < 0$ for $x>0$.



      If you continue taking the $x$ derivatives of $iH_0 ^{(1)} (ix)$, the sign of the derivatives alternates for $x>0$. My question is, how do I prove that for even $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) >0$ and for odd $n$, $frac{rm d ^n}{rm d x^n} big(iH^{(1)}_0 (ix)big) <0$?







      calculus complex-analysis bessel-functions






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      asked Nov 29 '18 at 16:43









      user207526user207526

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          We can transform the Hankel function into a modified Bessel function using the correspondence (DLMF) for $x>0$
          begin{equation}
          i{H^{(1)}_{0}}left(ixright)=frac{2}{pi}K_{0}left(xright)
          end{equation}

          Now, the $k$-th derivative can be obtained from the expression (DLMF) of that of the modified Bessel function:
          begin{align}
          &K_{0}^{(k)}left(xright)=\
          &frac{1}{2^{k}}left(e^{-ikpi}K_{-%
          k}left(xright)+{kchoose1}e^{-i(k-2)pi}K_{-k+2}left(x%
          right)+{kchoose2}e^{-i(k-4)pi}K_{-k+4}left(xright)+%
          cdots+e^{ikpi}K_{+k}left(xright)right)
          end{align}

          All phase factors of the sum equal $-1$ if $k$ is odd and $1$ if $k$ is even. As
          begin{align}
          frac{d^k}{dx^k}left[ i{H^{(1)}_{0}}left(ixright)right]&=frac{2}{pi}frac{d^k}{dx^k}left[K_{0}left(xright)right]
          end{align}

          Since $K_{-nu}(x)=K_nu(x)$ and $K_nu(x)$ is positive, the sign of the $k$-th derivative is the same as $(-1)^k$ as expected.






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            1 Answer
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            1 Answer
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            active

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            0














            We can transform the Hankel function into a modified Bessel function using the correspondence (DLMF) for $x>0$
            begin{equation}
            i{H^{(1)}_{0}}left(ixright)=frac{2}{pi}K_{0}left(xright)
            end{equation}

            Now, the $k$-th derivative can be obtained from the expression (DLMF) of that of the modified Bessel function:
            begin{align}
            &K_{0}^{(k)}left(xright)=\
            &frac{1}{2^{k}}left(e^{-ikpi}K_{-%
            k}left(xright)+{kchoose1}e^{-i(k-2)pi}K_{-k+2}left(x%
            right)+{kchoose2}e^{-i(k-4)pi}K_{-k+4}left(xright)+%
            cdots+e^{ikpi}K_{+k}left(xright)right)
            end{align}

            All phase factors of the sum equal $-1$ if $k$ is odd and $1$ if $k$ is even. As
            begin{align}
            frac{d^k}{dx^k}left[ i{H^{(1)}_{0}}left(ixright)right]&=frac{2}{pi}frac{d^k}{dx^k}left[K_{0}left(xright)right]
            end{align}

            Since $K_{-nu}(x)=K_nu(x)$ and $K_nu(x)$ is positive, the sign of the $k$-th derivative is the same as $(-1)^k$ as expected.






            share|cite|improve this answer


























              0














              We can transform the Hankel function into a modified Bessel function using the correspondence (DLMF) for $x>0$
              begin{equation}
              i{H^{(1)}_{0}}left(ixright)=frac{2}{pi}K_{0}left(xright)
              end{equation}

              Now, the $k$-th derivative can be obtained from the expression (DLMF) of that of the modified Bessel function:
              begin{align}
              &K_{0}^{(k)}left(xright)=\
              &frac{1}{2^{k}}left(e^{-ikpi}K_{-%
              k}left(xright)+{kchoose1}e^{-i(k-2)pi}K_{-k+2}left(x%
              right)+{kchoose2}e^{-i(k-4)pi}K_{-k+4}left(xright)+%
              cdots+e^{ikpi}K_{+k}left(xright)right)
              end{align}

              All phase factors of the sum equal $-1$ if $k$ is odd and $1$ if $k$ is even. As
              begin{align}
              frac{d^k}{dx^k}left[ i{H^{(1)}_{0}}left(ixright)right]&=frac{2}{pi}frac{d^k}{dx^k}left[K_{0}left(xright)right]
              end{align}

              Since $K_{-nu}(x)=K_nu(x)$ and $K_nu(x)$ is positive, the sign of the $k$-th derivative is the same as $(-1)^k$ as expected.






              share|cite|improve this answer
























                0












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                0






                We can transform the Hankel function into a modified Bessel function using the correspondence (DLMF) for $x>0$
                begin{equation}
                i{H^{(1)}_{0}}left(ixright)=frac{2}{pi}K_{0}left(xright)
                end{equation}

                Now, the $k$-th derivative can be obtained from the expression (DLMF) of that of the modified Bessel function:
                begin{align}
                &K_{0}^{(k)}left(xright)=\
                &frac{1}{2^{k}}left(e^{-ikpi}K_{-%
                k}left(xright)+{kchoose1}e^{-i(k-2)pi}K_{-k+2}left(x%
                right)+{kchoose2}e^{-i(k-4)pi}K_{-k+4}left(xright)+%
                cdots+e^{ikpi}K_{+k}left(xright)right)
                end{align}

                All phase factors of the sum equal $-1$ if $k$ is odd and $1$ if $k$ is even. As
                begin{align}
                frac{d^k}{dx^k}left[ i{H^{(1)}_{0}}left(ixright)right]&=frac{2}{pi}frac{d^k}{dx^k}left[K_{0}left(xright)right]
                end{align}

                Since $K_{-nu}(x)=K_nu(x)$ and $K_nu(x)$ is positive, the sign of the $k$-th derivative is the same as $(-1)^k$ as expected.






                share|cite|improve this answer












                We can transform the Hankel function into a modified Bessel function using the correspondence (DLMF) for $x>0$
                begin{equation}
                i{H^{(1)}_{0}}left(ixright)=frac{2}{pi}K_{0}left(xright)
                end{equation}

                Now, the $k$-th derivative can be obtained from the expression (DLMF) of that of the modified Bessel function:
                begin{align}
                &K_{0}^{(k)}left(xright)=\
                &frac{1}{2^{k}}left(e^{-ikpi}K_{-%
                k}left(xright)+{kchoose1}e^{-i(k-2)pi}K_{-k+2}left(x%
                right)+{kchoose2}e^{-i(k-4)pi}K_{-k+4}left(xright)+%
                cdots+e^{ikpi}K_{+k}left(xright)right)
                end{align}

                All phase factors of the sum equal $-1$ if $k$ is odd and $1$ if $k$ is even. As
                begin{align}
                frac{d^k}{dx^k}left[ i{H^{(1)}_{0}}left(ixright)right]&=frac{2}{pi}frac{d^k}{dx^k}left[K_{0}left(xright)right]
                end{align}

                Since $K_{-nu}(x)=K_nu(x)$ and $K_nu(x)$ is positive, the sign of the $k$-th derivative is the same as $(-1)^k$ as expected.







                share|cite|improve this answer












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                answered Nov 29 '18 at 21:10









                Paul EntaPaul Enta

                4,28611129




                4,28611129






























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