The local coordinate at a cusp #
For a positive width w, the usual local coordinate
z ↦ exp (2 π i z / w) maps the upper half-plane onto the punctured unit disc. Its fibres
are exactly the orbits of the translation subgroup w ℤ. Consequently it identifies the orbit
quotient of the upper half-plane by these translations with the punctured unit disc.
A periodic function need only be holomorphic above some height for boundedness to make its q-extension analytic at zero. This permits applying the same coordinate to functions with interior poles.
The construction reuses Mathlib's Function.Periodic.qParam; in particular, the normalization
of 2 π i / w agrees with the local parameter used for modular-form q-expansions. The analytic
extension criterion uses Function.Periodic.differentiableAt_cuspFunction_zero and Mathlib's
removable singularity theorem.
Main declarations #
TauCeti.UpperHalfPlane.qParamPuncturedUnitDisc: the width-wq-parameter with its range bundled.TauCeti.UpperHalfPlane.invQParamUpperHalfPlane: a chosen logarithmic lift/right inverse, valued in the upper half-plane.TauCeti.UpperHalfPlane.qParamPuncturedUnitDisc_eq_iff: two lifts have the same q-parameter exactly when they differ by an integral multiple of the width.TauCeti.UpperHalfPlane.cuspTranslationQuotientHomeomorph: the resulting homeomorphism from the translation-orbit quotient to the punctured unit disc.TauCeti.UpperHalfPlane.analyticAt_cuspFunction_zero_of_eventually_mdifferentiableAt: bounded functions holomorphic sufficiently high have a removable q-singularity.
References #
- Fred Diamond and Jerry Shurman, A First Course in Modular Forms, §2.4.
- Otto Forster, Lectures on Riemann Surfaces, §19.
A periodic function holomorphic at all sufficiently large heights and bounded at imaginary infinity has an analytic q-extension at zero. Interior poles below that height are allowed.
The q-parameter of positive width, regarded as a map from the upper half-plane to the punctured unit disc.
Equations
Instances For
The logarithmic lift of a point of the punctured unit disc to the upper half-plane.
Equations
- TauCeti.UpperHalfPlane.invQParamUpperHalfPlane w hw q = { coe := Function.Periodic.invQParam w ↑↑q, coe_im_pos := ⋯ }
Instances For
Every nonzero point of the unit disc has a logarithmic lift to the upper half-plane.
The q-parameter is holomorphic as a map into the punctured unit disc.
The image of a horodisc is the punctured disc of the corresponding exponential radius.
The q-parameter tends to zero through nonzero values as the height tends to infinity.
Multiplying by the kth integer power of the q-parameter cancels the opposing exponential
comparison and gives a function bounded at i∞. For positive width, nonnegative k controls
growth, while negative k controls decay.
Two points of the upper half-plane have the same width-w q-parameter exactly when one is
an integral-width translate of the other.
The orbit quotient of the upper half-plane by translations through integral multiples of a positive width.
Equations
Instances For
The orbit relation for integral-width translations is exactly equality of q-parameters.
The q-parameter from the upper half-plane to the punctured unit disc is an open quotient map.
The q-parameter descended to the width-translation quotient.
Equations
Instances For
The descended q-parameter is a homeomorphism.
The q-parameter identifies the width-translation quotient of the upper half-plane homeomorphically with the punctured unit disc.