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What does this connection between Chebyshev, Ramanujan, Ihara and Riemann mean?

It all started with Chris' answer saying returning paths on cubic graphs without backtracking can be expressed by the following recursion relation:

$$p_{r+1}(a) = ap_r(a)-2p_{r-1}(a)$$

$a$ is an eigenvalue of the adjacency matrix $A$. Chris mentions Chebyshev polynomials there. It was Will who found the generating function for the given recursion to be:

$$G(x,a)=\frac{1-x^2}{1-ax+2x^2} $$

and just recently Hamed put Chebychev back on the table:

$$ \frac{1-x^2}{1-ax +2x^2} \xrightarrow{x=t/\sqrt{2}}\frac{1-\frac{t^2}2}{1-2\frac{a}{\sqrt 8} t+t^2}=\left[1-\frac{t^2}{2}\right]\sum_{r=0}^\infty U_r\left(\frac{a}{\sqrt{8}}\right)t^r\\ =\sum_{r=0}^\infty \left(U_r\left(\frac{a}{\sqrt{8}}\right)-\frac12 U_{r-2}\left(\frac{a}{\sqrt{8}}\right)\right)t^r\\ $$ $$ \Rightarrow p_r(t)=\begin{cases}1 & \text{if $r=0$,}\\ 2^{r/2}U_r(t/\sqrt{8})-2^{(r-2)/2}U_{r-2}(t/\sqrt{8}) & \text{if $r\ge1$.}\end{cases} $$ The final line as taken from Will's community answer...

My question how to relate Ihara's $\zeta$ function and Chebyshev seems therefore mostly settled, but...:

Is it just a funny coincidence that the scaling factor of $\sqrt 8$ coincides with $\lambda_1\leq 2\sqrt 2$, which is the definition of cubic Ramanujan graphs.

And, there is another interesting thing:

As observed by Sunada, a regular graph is a Ramanujan graph if and only if its Ihara zeta function satisfies an analogue of the Riemann hypothesis.

What does this connection between Chebyshev, Ramanujan, Ihara and Riemann mean?

EDIT

I thought maybe something like a corollary could be possible:

  1. For Ramanujan graphs, the Ihara $\zeta$ function can be related to Chebyshev functions of the second kind, since the scaled eigenvalues of $A$ lie inside the range of convergence.
  2. A Ramanujan graph $G$ obeys the Riemann Hypothesis.
  3. Roots of the Ihara $\zeta$ function lie on the critical strip.
  • The bunch of people above have contributed to $1\leftarrow 2$.
  • $2 \leftrightarrow 3$ is proven here: Eigenvalues are of the form $\lambda=2\sqrt 2\cos(b\log 2)$
  • $3\overset{\rightarrow ?}{\leftarrow} 1$ would be nice...
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