Fiber primes of an integral extension Created 2026-09-24 Updated 2026-09-24
For an integral extension and , localization gives a bijection
It combines the prime ideal correspondence for localization with the contraction of a maximal ideal under an integral extension.
Put and define
where acts on through the given inclusion. By the prime ideal correspondence for localization, primes of correspond to primes of satisfying , equivalently .
The localized extension remains integral. If , then
is an integral domain integral over the field . An integral domain integral over a field is a field, so is maximal.
Conversely, if is maximal in , the contraction of a maximal ideal under an integral extension is maximal in the local ring , hence equals . Contracting once more to gives . Extension and contraction are inverse under localization, proving the required fiber primes of an integral extension bijection.
Let be maximal in and let be its contraction. The ideal is maximal and contains . It is disjoint from : if with , then . The prime ideal correspondence for localization therefore defines the proper ideal , and
is a field. Thus is maximal.
Conversely, let be the contraction to of a maximal ideal of . Then is maximal among ideals disjoint from . Since is disjoint from —otherwise an equation would put —maximality gives . If a proper ideal strictly contained in a maximal ideal of , then would also contain and hence remain disjoint from , a contradiction. Thus is maximal and contains .
The two standard extension-contraction bijections, first for and then for , now give inverse maps
Because , the localization remains an integral domain. Part (a) makes it Noetherian. Integral closedness is preserved by localization: if in the common fraction field is integral over , clearing the finitely many denominators in a monic equation shows that is integral over for some , whence and .
The prime ideal correspondence for localization shows that every chain of primes in comes from a chain in , so
If its dimension is one, it is a Noetherian integrally closed domain of dimension one and hence a Dedekind domain. If its dimension is zero, its zero ideal is maximal, so the domain is a field. This proves the Localization of a Dedekind domain alternative.