Fraction fields of localizations, polynomial rings and finite extensions #
Main results #
IsFractionRing.liftOfLocalization: a nonzero localization of a domain embeds compatibly in any fraction field of the domain, which is then a fraction field of the localization (IsFractionRing.isFractionRing_liftOfLocalization).MvPolynomial.coeffFractionRingEmbedding: a fraction field of a coefficient domainAembeds canonically in a fraction field ofMvPolynomial σ A, compatibly withAand its ground field.MvPolynomial.fractionRingCoeffMap,MvPolynomial.isFractionRing_fractionRingCoeffMap: enlarging the coefficients to their fraction field does not change the fraction field of a polynomial ring.IsFractionRing.exists_ne_zero_mul_mem_range_of_finite: a finite extension of domains with a common fraction field has a nonzero conductor element.
The elements of the submonoid of a nontrivial localization are nonzero.
A localization of a domain embeds compatibly in any fraction field of the domain.
Equations
Instances For
The embedding liftOfLocalization M of the localization S into a fraction field F of R
restricts to the algebra map R → F along R → S.
A fraction field of a domain is a fraction field of each of its nonzero localizations.
The coefficients embed in a fraction field of a polynomial ring over a domain.
The embedding of a fraction field of the coefficients into a fraction field of the polynomial ring.
Instances For
The embedding coeffFractionRingEmbedding of a fraction field F of A into E sends the
image of x : A in F to the image of x in E.
With the F-algebra structure on E given by coeffFractionRingEmbedding, the rings A, F
and E form a scalar tower.
Extend polynomial coefficients inside the ambient fraction field.
Equations
- MvPolynomial.fractionRingCoeffMap = MvPolynomial.eval₂Hom (algebraMap K F) fun (i : σ) => (algebraMap (MvPolynomial σ A) F) (MvPolynomial.X i)
Instances For
Composing fractionRingCoeffMap with the coefficient map MvPolynomial σ A → MvPolynomial σ K
gives the algebra map MvPolynomial σ A → F.
The constructed coefficient extension realizes the same ambient field as a fraction field after coefficient localization.
A common nonzero denominator for a finite birational extension.