Consider the pattern of the parity of the binomial numbers. Color the even numbers white and odd numbers black. You get a Sierpinski Triangle.
We will prove this using spacetime-geometric reasoning. It would help a lot if you have done some geometry of special relativity.
Define the parity function $f(t, n) = C(t, n) \mod 2$, defined on $\mathbb{N}\times\mathbb{Z}$.
We can consider $f(t, n)$ as encoding a 1-d celluar automata, with $t \ge 0, n \in \mathbb{Z}$. Then we have the evolution rule:
$$ f(t+1, n) = f(t, n) + f(t, n-1) \mod 2$$
This is just the Rule 60 celluar automata.
The state of any cell $n$ at time $t$ is determined by any constant-time-surface across its past lightcone. This is essentially a discrete version of physicist's idea of "past Cauchy surface": The state of any point in spacetime is determined by any surface that cuts through its past lightcone.
Lemma: for any cell, if all cells in any of its past Cauchy surface are dead, then that cell is also dead.
Proof: induct on $\Delta t$, how far in the past that Cauchy surface is.
Now begin the world with a single living cell at $n=0, t=0$. For cell at $n < 0$ or $n > t$, their past-Cauchy-surfaces at $t=0$ are all dead, so they are also dead.
Now induct to show Sierpinski.
At time $2^k - 1$, by induction, there is a solid row from $n = 0$ to $n = 2^k - 1$. So at time $2^k$, there is a big die-off, leaving only living cells at $n = 0$ and $2^k$.
At time $t + 2^k$, consider a cell at $0 \le n \le 2^k - 1$. Its relation to its past Cauchy surface at time $2^k$ are exactly the same as the relation of cell $n$ at time $t$ with its past Cauchy surface at time $0$. Same for a cell at $ n + 2^k$.
QED
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