The sinc function is defined by sinc(*x*) = sin(*x*)/*x*. Philip Woodward introduced the name of the function in 1952, saying it “occurs so often in Fourier analysis and its applications that it does seem to merit some notation of its own.”

Here’s an elegant equation involving the integrals of the sinc function:

When I ran across this recently I wondered two things: How hard is it to compute these two integrals? What are the corresponding results for the jinc function? The jinc function is analogous to sinc, but using a Bessel function in place of sine: jinc(*x*) = *J*_{1}(*x*)/*x*.

The Fourier transform of the box function, the function box(*x*) that is 1 on the interval [-1/2, 1/2] and zero everywhere else, is sinc(π ω). (That’s one of the reasons sinc comes up so often in Fourier analysis, as Woodward observed.) So the Fourier transform of sinc(*x*) is π box(π *x*). The integral of a function is the value of its Fourier transform at zero, so sinc integrates to π. [1]

By Plancherel’s theorem, the integral of sinc^{2}(*x*) is the integral of it’s Fourier transform squared, which equals π.

[There are several conventions for defining the Fourier transform. Here I’m using what I call the (-1, τ, 1) definition in these notes. See that page for other conventions and how to convert between them.]

Now for the jinc function. It also has a simple Fourier transform: *f*(ω) = 2 √(1 – (2πω)) for |*x*| < 1/2π and zero otherwise. As above, we can compute the integral of jinc over the real line by evaluating its Fourier transform at 0, which equals 2.

Also as above, the integral of jinc^{2} is the integral of its Fourier transform squared, which works out to 8/3π.

**Update**: See the next post for the analogous relations for sums.

## More on sinc and jinc functions

[1] You may have a couple objections to this calculation. I found the Fourier transform of the box function was sinc, then concluded that the transform of sinc is the box function. But applying the Fourier transform twice doesn’t give you the original function back, right? When you transform *f*(*x*) twice you get *f*(-*x*), but the functions involved here are even, so *f*(-*x*) = *f*(*x*).

OK, but you may still have another objection: the sinc function does not have bounded *L*^{1} norm, so you can’t just take it’s Fourier transform. True, but you can justify the transform in terms of *L*^{2} theory or distribution theory.

It’s also easy to show that the integral of sinc(x-a)*sinc(x-b) over all x is just pi * sinc(a-b), (for real a,b), which reduces to your result for sinc in the a==b case. (Just use the fact that sinc is essentially the Fourier transform of an indicator function for an interval centered on the origin.)

Note for jinc, the equivalent “shifting” formula is not as straightforward.

Although jinc is similar to sinc in that occurs naturally as the 2-D Fourier transform of an indicator for a circular disk centered on the origin. The jinc appears after transforming to polar coordinates. There is a natural “shifting” formula in Cartesian coordinates whenever the indicator region has reflection symmetry, but turning out an equivalent formula for the jinc from this fact

seems to be a bit of a mess.

Closed formula for the definite integral over the interval

(-inf, inf) of the nth power of the sinc function is derived in my paper “Computations of the inner products of some multivariate splines” (see page 109). This work appears in

Splines in Numerical Analysis (Proc. Conf. Weissig), Vol. 52 (J. Schmidt and H. Spath, Eds.), 97-110, Akademie-Verlag, Berlin , 1989.

Thanks, Edward. That sounds interesting.

It would be nice to have the values of integrals of each lobe, i.e. integrals between 0 and multiples of pi. Anyone knows of such a table?

Luca, please see my latest post for an answer to your question.

https://www.johndcook.com/blog/2019/12/31/sinc-jinc-lobes/