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Schwarz triangle function

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In mathematics, the Schwarz triangle tessellation was introduced by H. A. Schwarz as a way of tessellating the hyperbolic upper half plane by a Schwarz triangle, i.e. a geodesic triangle in the upper half plane with angles which are either 0 or of the form π over a positive integer greater than one. Through successive hyperbolic reflections in its sides, such a triangle generates a tessellation of the upper half plane (or the unit disk after composition with the Cayley transform). The hyperbolic refections generates a discrete group, with an orientation-preserving normal subgroup of index two. Each such tessellation yields a conformal mapping of the upper half plane onto the interior of the geodesic triangle, generalizing the Schwarz–Christoffel mapping, with the upper half plane replacing the complex plane. The corresponding inverse function, first defined by Schwarz, solved the problem of uniformization a hyperbolic triangle and is called the Schwarz triangle function.

Through the theory of complex ordinary differential equations with regular singular points and the Schwarzian derivative, the triangle function can be expressed as the quotient of two solutions of a hypergeometric differential equation with real coefficients and singular points at 0, 1 and ∞. By the Schwarz reflection principle, the reflection group induces an action on the two dimensional space of solutions. On the orientation-preserving normal subgroup, this two-dimensional representation corresponds to the monodromy of the ordinary differential equation and induces a group of Möbius transformations on quotients of hypergeometric functions.

As the inverse function of such a quotient, the triangle function is an automorphic function for this discrete group of Möbius transformations. This is a special case of a general scheme of Henri Poincaré that associates automorphic forms with ordinary differential equations with regular singular points. In the special case of ideal triangles, where all the angles are zero, the tessellation corresponds to the Farey tessellation and the triangle function yields the modular lambda function.


Hyperboloid and Beltrami-Klein models

Geometric relations between Poincaré disk model, hyperboloid model and Beltrami-Klein model

In this section two different models are given for hyperbolic geometry on the unit disk or equivalently the upper half plane.[1]

The group G = SU(1,1) is formed of matrices

with

It is a subgroup of Gc = SL(2,C), the group of complex 2 × 2 matrices with determinant 1. The group Gc acts by Möbius transformations on the extended complex plane. The subgroup G acts as automorphisms of the unit disk D and the subgroup G1 = SL(2,R) acts as automorphisms of the upper half plane. If

then

since the Möbius transformation corresponding M is the Cayley transform carrying the upper half plane onto the unit disk and the real line onto the unit circle.

The Lie algebra of SU(1,1) consists of matrices

with x real. Note that X2 = (|w|2x2) I and

The hyperboloid in is defined by two conditions. The first is that det X = 1 or equivalently Tr X2 = –2.[2] By definition this condition is preserved under conjugation by G. Since G is connected it leaves the two components with x > 0 and x < 0 invariant. The second condition is that x > 0. For brevity, write X = (x,w).

The group G acts transitively on D and and the points 0 and (1,0) have stabiliser K consisting of matrices

with |ζ| = 1. Polar decomposition on D implies the Cartan decomposition G = KAK where A is the group of matrices

Both spaces can therefore be identified with the homogeneous space G/K and there is a G-equivariant map f of onto D sending (1,0) to 0. To work out the formula for this map and its inverse it suffices to compute g(1,0) and g(0) where g is as above. Thus g(0) = β/α and

so that

recovering the formula

Conversely if z = iw/(x + 1), then |z|2 = (x – 1)/(x + 1), giving the inverse formula

This correspondence extends to one between geometric properties of D and . Without entering into the correspondence of G-invariant Riemannian metrics,[a] each geodesic circle in D corresponds to the intersection of 2-planes through the origin, given by equations Tr XY = 0, with . Indeed, this is obvious for rays arg z = θ through the origin in D—which correspond to the 2-planes arg w = θ—and follows in general by G-equivariance.

The Beltrami-Klein model is obtained by using the map F(x,w) = w/x as the correspondence between and D. Identifying this disk with (1,v) with |v| < 1, intersections of 2-planes with correspond to intersections of the same 2-planes with this disk and so give straight lines. The Poincaré-Klein map given by

thus gives a diffeomorphism from the unit disk onto itself such that Poincaré geodesic circles are carried into straight lines. This diffeomorphism does not preserve angles but preserves orientation and, like all diffeomorphisms, takes smooth curves through a point making an angle less than π (measured anticlockwise) into a similar pair of curves.[b] In the limiting case, when the angle is π, the curves are tangent and this again is preserved under a diffeomorphism. The map K yields the Beltrami-Klein model of hyperbolic geometry. The map extends to a homeomorphism of the unit disk onto itself which is the identity on the unit circle. Thus by continuity the map K extends to the endpoints of geodesics, so carries the arc of the circle in the disc cutting the unit circle orthogonally at two given points on to the straight line segment joining those two points. The use of the Beltrami-Klein model corresponds to projective geometry and cross ratios. (Note that on the unit circle the radial derivative of K vanishes, so that the condition on angles no longer applies there.)[3][4]

The group G1 = SL(2,R) is formed of real matrices

with The action is by Möbius transformations on the upper half-plane. The Lie algebra of G1 is , the space of 2 x 2 real matrices of trace zero,

By transport of construction — conjugating by C — the symmetric bilinear form Tr ad(X)ad(Y) = 4 Tr XY is invariant under conjugation and has signature (2,1). As above X2 = (x2 + y2t2) I and

By Sylvester's law of inertia,[5] the Killing form (or Cartan-Killing form) is, up to equivalence, the unique symmetric bilinear form of signature (2,1) with corresponding quadratic form –x2y2 +t2; and G / {±I} or equivalently G1 / {±I} can be identified with SO(2,1).

Conformal mapping of Schwarz triangles

In this section Schwarz's explicit conformal mapping from the unit disc or the upper half plane to the interior of a Schwarz triangle will be constructed as the ratio of solutions of a hypergeometric ordinary differential equation, following Carathéodory (1954, pp. 129–194), Nehari (1975, pp. 198–209, 308–332) and Hille (1976, pp. 371–401). The classical account of Ince (1944, pp. 389–395) has an account of the monodromy of second order complex order differential equations with regular singular points. The limiting case of ideal triangles, the Farey series and the modular lambda function is explained in Ahlfors (1966, pp. 254–274), Chandrasekharan (1985, pp. 108–121), Mumford, Series & Wright (2015) and Hardy & Wright (2008).

The Schwarz triangle function or Schwarz s-function is a function that conformally maps the upper half plane to a triangle in the upper half plane having lines or circular arcs for edges. Let πα, πβ, and πγ be the interior angles at the vertices of the triangle. If any of α, β, and γ are greater than zero, then the Schwarz triangle function can be given in terms of hypergeometric functions as:

where a = (1−α−β−γ)/2, b = (1−α+β−γ)/2, c = 1−α, a′ = ac + 1 = (1+α−β−γ)/2, b′ = bc + 1 = (1+α+β−γ)/2, and c′ = 2 − c = 1 + α. This mapping has singular points at z = 0, 1, and ∞, corresponding to the vertices of the triangle with angles πα, πγ, and πβ respectively. At these singular points,

This formula can be derived using the Schwarzian derivative.

This function can be used to map the upper half-plane to a spherical triangle on the Riemann sphere if α + β + γ > 1, or a hyperbolic triangle on the Poincaré disk if α + β + γ < 1. When α + β + γ = 1, then the triangle is a Euclidean triangle with straight edges: a = 0, , and the formula reduces to that given by the Schwarz–Christoffel transformation. In the special case of ideal triangles, where all the angles are zero, the triangle function yields the modular lambda function.

See also

Notes

  1. ^ The Poincaré metric on the disk corresponds to the restriction of the G-invariant pseudo-Riemannian metric dx2dw2 to the hyperboloid.
  2. ^ The condition on tangent vectors x, y is given by det (x,y) ≥ 0 and is preserved because the determinant of the Jacobian is positive.

References

  1. ^ See:
  2. ^ Note that the Killing form B(X,Y) = Tr ad X ad Y = 4 Tr XY.Helgason 1978
  3. ^ Iversen 1992
  4. ^ Magnus 1974
  5. ^ Ratcliffe 2019, pp. 52–56
  6. ^ Lee, Laurence (1976). Conformal Projections based on Elliptic Functions. Cartographica Monographs. Vol. 16. University of Toronto Press. ISBN 9780919870161. Chapters also published in The Canadian Cartographer. 13 (1). 1976.

Sources

Further reading

  • Ford, Lester R. (1951) [1929], Automorphic Functions, American Mathematical Society, ISBN 0821837419 {{citation}}: ISBN / Date incompatibility (help)
  • Lehner, Joseph (1964), Discontinuous groups and automorphic functions, Mathematical Surveys, vol. 8, American Mathematical Society. (Note that Lehner has pointed out that his proof of Poincaré's polygon theorem is incomplete. He has subsequently recommended de Rham's 1971 exposition.)
  • Sansone, Giovanni; Gerretsen, Johan (1969), Lectures on the theory of functions of a complex variable. II: Geometric theory, Wolters-Noordhoff
  • Series, Caroline (1985), "The modular surface and continued fractions", Journal of the London Mathematical Society, 31: 69–80, doi:10.1112/jlms/s2-31.1.69
  • Thurston, William P. (1997), Silvio Levy (ed.), Three-dimensional geometry and topology. Vol. 1., Princeton Mathematical Series, vol. 35, Princeton University Press, ISBN 0-691-08304-5