If and is observed, the maximum-likelihood estimate of is zero. A one-sided upper confidence bound solves , so . For large , , giving approximately at 95% confidence. This describes uncertainty after no observed events, rather than proving that the underlying probability is zero. It assumes independent observations with a common event probability; clustered data require a different uncertainty calculation.
At fixed odd , the zero-temperature canonical ensemble equally weights the ground states of an antiferromagnetic Ising ring. The single frustrated bond in an antiferromagnetic Ising ring lies on a chosen -bond path with probability . The Ising spin product is if the path excludes that bond and if it includes it, proving the displayed two-point correlation function. The loss of staggered alignment upon averaging persists at zero temperature and is caused by geometric frustration, rather than a positive density of thermal defects. The expression remains symmetric under for odd .