Unramified finite places over Frobenius-twist fields #
The Galois group of the exact constant extension over a Frobenius-twist field is the cyclic subgroup generated by the twist. Restriction to the enlarged constants is injective on this subgroup. An inertia automorphism acts trivially on every residue class, hence in particular on the embedded constant field. It therefore lies in the kernel of constant restriction and must be the identity. Thus every finite place is unramified in the exact constant extension over a twist field.
The algebra structure from C to N used in the exact constant extension frobenius
twist finite place unramified construction.
Instances For
The canonical twist generates the full Galois group over its fixed field. This is a direct consequence of defining that fixed field from the cyclic subgroup generated by the ambient twist.
If one generator of a relative Galois group fixes a top finite place, then generation, unramifiedness, and maximal possible top degree force the restricted finite place to have degree one.
Conversely, under the same degree-divisibility hypothesis used for the unique-lift theorem, every lift of a rational finite place has top degree equal to the relative field degree.
Rational finite places are equivalent to generator-fixed top finite places of relative-degree-sized absolute degree, once the relative extension is unramified and every top degree is divisible by the relative degree.
Equations
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Instances For
Relative automorphisms over two intermediate fields induce the same action on top finite places when their underlying top-field maps agree.
Every finite place of the exact constant extension is unramified over a Frobenius-twist fixed field, provided the twist has the full constant-extension order.
A top finite place of degree [S : C] fixed by the canonical twist
descends to a rational finite place of the Frobenius-twist fixed field.
The canonical twist over its fixed field and the ambient twist over
C(X) induce exactly the same action on finite places.
Ambient fixedness by the Frobenius twist is therefore the exact fixedness condition needed for descent to a rational twist-field place.
Rational finite places of the Frobenius-twist field are exactly the
degree-[S : C] top finite places fixed by the ambient Frobenius twist.
Equations
- One or more equations did not get rendered due to their size.