I got curious about this integral because we have the following identity:
2π∫π/20cos(xcost)dt=J0(x)
So we have an interesting (if useless) symmetry:
∫π/20J0(cosx)dx=2π∫π/20∫π/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=√π2∞∑k=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=0∞∑n=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=0k∑m=0(−1)km!2(k−m)!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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