Amplification by Read-Once Formulas

Moore and Shannon have shown that relays with arbitrarily high reliability can be built from relays with arbitrarily poor reliability. Valiant used similar methods to construct monotone read-once formulas of size $O(n^{\alpha+2})$ (where $\alpha=\log_{\sqrt{5}-1}2\simeq 3.27$) that amplify $(\psi-\frac{1}{n},\psi+\frac{1}{n})$ (where $\psi=(\sqrt{5}-1)/2\simeq0.62$) to $(2^{-n},1-2^{-n})$ and deduced as a consequence the existence of monotone formulas of the same size that compute the majority of $n$ bits. Boppana has shown that any monotone read-once formula that amplifies $(p-\frac{1}{n},p+\frac{1}{n})$ to $(\frac{1}{4},\frac{3}{4})$ (where $0We extend Boppana's results in two ways. We first show that his two lower bounds hold for general read-once formulas, not necessarily monotone, that may even include exclusive-or gates. We are then able to join his two lower bounds together and show that any read-once, not necessarily monotone, formula that amplifies $(p-\frac{1}{n},p+\frac{1}{n})$ to $(2^{-n},1-2^{-n})$ has size $\Omega(n^{\alpha+2})$. This result does not follow from Boppana's arguments, and it shows that the amount of amplification achieved by Valiant is the maximal achievable using read-once formulas. In a companion paper we construct monotone read-once contact networks of size $O(n^{2.99})$ that amplify $(\frac{1}{2}-\frac{1}{n},\frac{1}{2}+\frac{1}{n})$ to $(\frac{1}{4},\frac{3}{4})$. This shows that Boppana's lower bound for the first amplification stage does not apply to contact networks, even if they are required to be both monotone and read-once.