- I don't know what is given as data, but if the positions of turned on lamps is given first you should extract all contiguous extinguished lightbulbs.
Example:
000111010100110000
S= {{1,2,3},{7},{9},{11,12},{15,16,17,18}}
Next get the cardinals: |S|={3,1,1,2,4}
If you try to visualise the problem as a set of permutations, solution is just a multinomial distribution $\binom{n}{3,4,(1-1),(1-1),(2-1)}$
For a set of cardinals $|S|=\{x_0,x_1,x_2,x_3,x_4,...x_i\}$
Solution is $\binom{n}{x_0,\sum_j(x_1-j-1,j_1),\sum_j(x_2-j-2,j_2),...,x_i}$
$$=\sum_{j_1,j_2,...=0}\frac{n!}{x_0!(x_1-j_1-1)!j_1!(x_2-j_2-1)!j_2!...!x_i!}$$
Where $n$ is the number of extinct bulbs=$x_0+x_1+...x_n$.
Explanation:
For instance, a particular set of $x_0,x_1-j_1,j_1,x_2-j_2,j_2,...x_i$ and n extinct bulbls, permutations of these elements just notes the order of choosing either of these contiguous sub-lists, the act of choosing a sublist is visioned as clicking the edgemost switch of aligned ones that are all switched off, why $x_j-j-1$ ? because a set of complete $x_j$ encompasses one that is arranged with different list, so removing 1 from both opposite subsets as reserving a "nobody's land" of length=1 at the middle corrects the problem of duplicate choices.
Edit: After a bit of thinking i realised that a coincidence of choosing the no-cross line fixed between opposite subsets before $j$ or $x-j-1$ elements must be excluded, hence divided upon.
$S=\sum_{j_1,j_2,...=0}\frac{n!}{x_0!(x_1-j_1-1)!j_1!(j_1-1)(x_1-j_1-2)(x_2-j_2-1)!j_2!(j_2-1)(x_2-j_2-2)...!x_i!}$=$$\sum_{j_1,j_2,...=0}\frac{n!}{x_0!(x_1-j_1-1)!j_1!(x_2-j_2-1)!j_2!...!x_i!*(j_1-1)(x_1-j_1-2)(j_2-1)(x_2-j_2-2)...}$$