Problem set 3

Let S1S^1 be the unit circle. We work on C(S1)\mathscr{C}^{\infty}(S^1), the smooth functions on the circle. In this note we identify S1S^1 with [0,2π][0,2\pi] for simplicity. Let (f,g)=12π02πf(x)g(x)dx(f,g) = \frac{1}{2\pi}\int_{0}^{2\pi} f(x)\overline{g(x)} dx be the inner product.

Let D:C(S1)C(S1)D:\mathscr{C}^{\infty}(S^1)\mapsto \mathscr{C}^{\infty}(S^1) be the differential operator given by fiddxff\mapsto -i\frac{d}{dx}f, it is a linear operator on C(S1)\mathscr{C}^{\infty}(S^1). DD is called the Dirac operator, it satisfies the property that D2=ΔD^2 = \Delta.

Problem 1.

(1) Show that DD is self adjoint, i.e. (Df,g)=(f,Dg)(Df,g) = (f,Dg) for f,gC(S1)f,g\in \mathscr{C}^{\infty}(S^1).

(2) Show that D2=ddx2D^2 = \frac{d}{dx^2}, which is the 1-dimensional Laplacian operator. Show that einxe^{ i n x} are eigenfunctions of DD, with eigenvalue nn.

Problem 2.

For sCs\in \mathbb{C}, let D+sD+s denote the operator D+sID+sI, so that (D+s)(f)=Df+sf(D+s)(f) = Df + sf. Show that for sC/Zs\in \mathbb{C}/\mathbb{Z}, D+sD+s is invertible.

Problem 3.

If you have done right in problem 2, you will get

(D+s)1f=n=+f^(n)n+seinx. (D+s)^{-1}f = \sum_{n = -\infty}^{+\infty}\frac{\hat{f}(n)}{n+s} e^{inx}.

Find a function gg such that (D+s)1(f)=fg(D+s)^{-1}(f) = f*g.

Problem 4.

If you are comfortable with convolution theorem, you would find g(x)=n=+1n+seinxg(x) = \sum_{n = -\infty}^{+\infty}\frac{1}{n+s}e^{inx} in problem 3.

(1) Show that nZ1n+seinx\sum_{n\in \mathbb{Z}}\frac{1}{n+s}e^{inx} is the Fourier series of πsinπsei(πx)s\frac{\pi}{\sin \pi s}e^{i(\pi-x)s}, conclude that g(x)=πsinπsei(πx)sg(x) = \frac{\pi}{\sin \pi s} e^{i(\pi -x)s}.

(2) Show that n=+1n+s=πcot(πs)=πi2πik=0+e2πims\sum_{n=-\infty}^{+\infty}\frac{1}{n+s} = \pi \cot(\pi s) = \pi i - 2\pi i \sum_{k= 0}^{+\infty}e^{2\pi i ms}. Note that this is a key identity to derive the Fourier series of Eisenstein series. See also page 5 of Diamond-Shurman A first course to modular forms.

(3) Show that if sTs\in \mathbb{T} and s0s \neq 0, then n=+1n+s2=π2sin(πs)2\sum_{n = -\infty}^{+\infty}\frac{1}{|n+s|^2} = \frac{\pi^2}{|\sin(\pi s)|^2}.

Problem 5

Let ff be continuous at everywhere on the circle except for a jump discontinunity at 0.

(1) Let σ(x)=limNσNf(x)\sigma(x) = \lim_{N\to \infty}\sigma_Nf(x). Show that σ(x)={f(x),x0f(0+)+f(0)2,x=0\sigma(x) = \begin{cases} f(x), x\neq 0\\ \frac{f(0^+)+f(0^-)}{2}, x = 0 \end{cases}

(2) We know that if SN(f)S_N(f) converges pointwise to FF, then σNf\sigma_N f converges pointwise to the same FF. Show that the reverse holds when cn=o(1/n)|c_n| = o(1/n), where cnc_n is the Fourier coefficients of ff.

(3) Conclude that when ff is piecewise C1\mathscr{C}^1 on the circle with jump discontinunity at 0, then SN(f)(0)f(0)+f(0+)2S_N(f)(0)\to \frac{f(0^-)+f(0^+)}{2}. Apply this result to problem 4(2).

References
  1. (2005). In Graduate Texts in Mathematics. Springer New York. 10.1007/978-0-387-27226-9
  2. Chernoff, P. R. (1980). Pointwise Convergence of Fourier Series. The American Mathematical Monthly, 87(5), 399–400. 10.1080/00029890.1980.11995049