Thursday, 8 May 2014

sequences and series - Prove intpi/20J0(cosx)dx=fracpi2left(J0left(frac12right)right)2



I got curious about this integral because we have the following identity:



2ππ/20cos(xcost)dt=J0(x)



So we have an interesting (if useless) symmetry:



π/20J0(cosx)dx=2ππ/20π/20cos(cosxcost) dt dx=π/20J0(cost)dt




Wolfram Alpha doesn't show a closed form for this integral. However, if we use the series for the Bessel function:



J0(x)=k=0(1)kx2k4kk!2



And the known closed form for the family of integrals:



π/20cos2k(x)dx=π2Γ(k+12)k!



We obtain:




π/20J0(cosx)dx=π2k=0(1)kΓ(k+12)4kk!3



Wolfram Alpha evaluates this series, giving a closed form for the integral:



π/20J0(cosx)dx=π2(J0(12))2=1.3834405



This agrees with the numerical value. However, I have not been able to show this myself.





How do we prove this closed form? Is there a more general case, involving Bessel functions of order n?



Answer



J0(x)2=m=0n=0(1)m+nm!2n!2x2(m+n)22(m+n)



or, looking at coefficients of x2k, i.e., m+n=k:



J0(x)2=k=0km=0(1)km!2(km)!2x2k22k



Now,




\sum_{m=0}^k \frac{1}{m!^2 (k-m)!^2} = \frac1{k!^2} \binom{2 k}{k}



Thus,



J_0 \left ( \frac12 \right )^2 = \sum_{k=0}^{\infty} \frac{(-1)^k (2 k)!}{2^{4 k} k!^4}



which you will find is equivalent to the sum you have above.



NB




\Gamma \left (k+\frac12 \right ) = \frac{(2 k)! \sqrt{\pi}}{2^{2 k} k!}


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