The q-coordinate chart at a cusp of the compactified quotient #
Let Γ ≤ PSL(2, ℝ) be discrete and D a normalized cusp datum of Γ with scaling σ and width
w. For a height A ≥ w the horodisc of height A at D is precisely invariant under the cusp
stabilizer, so the q-coordinate q(z) = exp (2 * π * I * σ(z) / w) descends to the image of the
horodisc in the coarse quotient Γ \ ℍ, and it extends by q = 0 to the cusp orbit adjoined in
the compactified quotient. This file packages this extension as an open partial homeomorphism
Subgroup.CompactifiedQuotient.cuspChart D hA from the compactified quotient to ℂ: its source
is the cusp neighbourhood cuspNhd D A and its target the disc of radius cuspRadius D A, the
exponential exp (-2 * π * A / w) of the height. On the target, the inverse sends 0 to the cusp
orbit and a nonzero q to the orbit of the logarithmic lift σ⁻¹ • invQParam w q.
Continuity at the cusp orbit is the fact that the q-coordinate tends to 0 along the cusp and,
conversely, that the logarithmic lift of a small q lies in a high horodisc. Continuity away from
the cusp orbit comes from the open quotient map qCoordinate D onto the punctured unit disc.
The compatibility of these charts with the atlas of the coarse quotient, and the resulting Riemann
surface structure on the compactified quotient, are not part of this file.
Main declarations #
Subgroup.CompactifiedQuotient.cuspRadius: the radiusexp (-2 * π * A / w)of the q-disc corresponding to the horodisc of heightA.Subgroup.CompactifiedQuotient.cuspChart: the cusp chart, withSubgroup.CompactifiedQuotient.cuspChart_ofCuspandSubgroup.CompactifiedQuotient.cuspChart_ofQuotient_mkcomputing it on its source, andSubgroup.CompactifiedQuotient.cuspChart_symm_zero,Subgroup.CompactifiedQuotient.cuspChart_symm_coordinateandSubgroup.CompactifiedQuotient.cuspChart_symm_of_ne_zerocomputing its inverse on its target.
The underlying total maps of the chart and its inverse are implementation details: outside the source and target their values are junk, so they are private.
References #
- Fred Diamond and Jerry Shurman, A First Course in Modular Forms, Graduate Texts in Mathematics 228, Springer, 2005, §2.4.
- Otto Forster, Lectures on Riemann Surfaces, Graduate Texts in Mathematics 81, Springer, 1981, §19.
- Svetlana Katok, Fuchsian Groups, Chicago Lectures in Mathematics, University of Chicago Press, 1992, §4.2.
The radius of the q-disc #
The radius exp (-2 * π * A / w) of the punctured q-disc onto which the horodisc of height A
is mapped by the q-coordinate of a cusp datum of width w.
Instances For
The radius of the q-disc tends to zero as the height tends to infinity.
A horodisc is the inverse image of the q-disc of the corresponding radius.
The forward map #
The total map underlying the cusp chart. Its values off the cusp neighbourhood are junk, so it and its lemmas are private.
The inverse map #
The total map underlying the inverse of the cusp chart. Its values off the unit disc are junk, so it and its lemmas are private.
Continuity #
The chart #
The cusp chart of the compactified quotient at the cusp datum D and a height A at least
its width. Its source is the cusp neighbourhood cuspNhd D A and its target the disc of radius
cuspRadius D A; it sends the cusp orbit to 0 and the orbit of a point z of the horodisc to
its q-coordinate coordinate D z.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The cusp chart sends its cusp orbit to 0.
The cusp chart sends the orbit of a point of the horodisc to its q-coordinate.
The inverse of the cusp chart sends 0 to the cusp orbit.
The inverse of the cusp chart sends the q-coordinate of a point of the horodisc to its orbit.
The inverse of the cusp chart sends a nonzero point q of its target to the orbit of the
logarithmic lift σ⁻¹ • invQParam w q.