Analytic functions are determined by their restrictions to lines #
A function analytic at p vanishes on a neighbourhood of p exactly when its restriction
t β¦ f (p + t β’ v) to every line through p vanishes on a neighbourhood of 0. The nontrivial
direction is the identity principle along each line: on a ball around p where f is analytic,
the restriction to the line through p and a point y of the ball is analytic on a disc
containing 0 and 1, so it vanishes at 1, that is at y.
In several complex variables this is the first step of putting a nonzero germ in general position:
some direction v has a restriction that does not vanish identically, and in linear coordinates
whose last axis is v the germ becomes regular in the last variable, as Weierstrass preparation
requires (AnalyticAt.exists_continuousLinearEquiv_analyticOrderAt_ne_top).
The name follows Mathlib's Mathlib.Analysis.Analytic.Uniqueness, where the identity principle
lives.
Main declarations #
AnalyticAt.eventuallyEq_zero_iff_forall_eventuallyEq_zero_comp_add_smul: an analytic function vanishes nearpexactly when all its restrictions to lines throughpvanish near0.AnalyticAt.exists_continuousLinearEquiv_analyticOrderAt_ne_top: after a linear change of coordinates, a function onE Γ πnot vanishing nearphas finite order in the last variable.
References #
- L. HΓΆrmander, An Introduction to Complex Analysis in Several Variables, Β§6.1.
- R. C. Gunning, H. Rossi, Analytic Functions of Several Complex Variables, Ch. II, Β§B.
An analytic function is determined near a point by its restrictions to lines. A function
analytic at p vanishes on a neighbourhood of p exactly when, for every direction v, the
restriction t β¦ f (p + t β’ v) vanishes on a neighbourhood of 0.
General position in the last variable. A function analytic at p on E Γ π that does not
vanish near p becomes regular in the last variable after a linear change of coordinates: there
are a continuous linear automorphism L and a point q with L q = p such that
t β¦ f (L (q.1, t)) has finite analytic order at q.2. The last axis is sent to a direction along
which the restriction of f does not vanish identically.