Upper half-plane

In mathematics, the upper half-plane, H,{\displaystyle {\mathcal {H}},} is the set of points (x,y){\displaystyle (x,y)} in the Cartesian plane with y>0.{\displaystyle y>0.} The lower half-plane is the set of points (x,y){\displaystyle (x,y)} with y<0{\displaystyle y<0} instead. Arbitrarily oriented half-planes can be obtained via a planar rotation. Half-planes are an example of two-dimensional half-space. A half-plane can be split in two quadrants.

Affine geometry

The affine transformations of the upper half-plane include

  1. shifts (x,y)(x+c,y){\displaystyle (x,y)\mapsto (x+c,y)}, cR{\displaystyle c\in \mathbb {R} }, and
  2. dilations (x,y)(λx,λy){\displaystyle (x,y)\mapsto (\lambda x,\lambda y)}, λ>0.{\displaystyle \lambda >0.}

Proposition: Let A{\displaystyle A} and B{\displaystyle B} be semicircles in the upper half-plane with centers on the boundary. Then there is an affine mapping that takes A{\displaystyle A} to B{\displaystyle B}.

Proof: First shift the center of A{\displaystyle A} to (0,0).{\displaystyle (0,0).} Then take λ=(diameter of B)/(diameter of A){\displaystyle \lambda =({\text{diameter of}}\ B)/({\text{diameter of}}\ A)}

and dilate. Then shift (0,0){\displaystyle (0,0)} to the center of B.{\displaystyle B.}

Inversive geometry

Definition:Z:={(cos2θ,12sin2θ)0<θ<π}{\displaystyle {\mathcal {Z}}:=\left\{\left(\cos ^{2}\theta ,{\tfrac {1}{2}}\sin 2\theta \right)\mid 0<\theta <\pi \right\}}.

Z{\displaystyle {\mathcal {Z}}} can be recognized as the circle of radius 12{\displaystyle {\tfrac {1}{2}}} centered at (12,0),{\displaystyle {\bigl (}{\tfrac {1}{2}},0{\bigr )},} and as the polar plot of ρ(θ)=cosθ.{\displaystyle \rho (\theta )=\cos \theta .}

Proposition:(0,0),{\displaystyle (0,0),}ρ(θ){\displaystyle \rho (\theta )} in Z,{\displaystyle {\mathcal {Z}},} and (1,tanθ){\displaystyle (1,\tan \theta )} are collinear points.

In fact, Z{\displaystyle {\mathcal {Z}}} is the inversion of the line {(1,y)y>0}{\displaystyle {\bigl \{}(1,y)\mid y>0{\bigr \}}} in the unit circle. Indeed, the diagonal from (0,0){\displaystyle (0,0)} to (1,tanθ){\displaystyle (1,\tan \theta )} has squared length 1+tan2θ=sec2θ{\displaystyle 1+\tan ^{2}\theta =\sec ^{2}\theta }, so that ρ(θ)=cosθ{\displaystyle \rho (\theta )=\cos \theta } is the reciprocal of that length.

Metric geometry

The distance between any two points p{\displaystyle p} and q{\displaystyle q} in the upper half-plane can be consistently defined as follows: The perpendicular bisector of the segment from p{\displaystyle p} to q{\displaystyle q} either intersects the boundary or is parallel to it. In the latter case p{\displaystyle p} and q{\displaystyle q} lie on a ray perpendicular to the boundary and logarithmic measure can be used to define a distance that is invariant under dilation. In the former case p{\displaystyle p} and q{\displaystyle q} lie on a circle centered at the intersection of their perpendicular bisector and the boundary. By the above proposition this circle can be moved by affine motion to Z.{\displaystyle {\mathcal {Z}}.} Distances on Z{\displaystyle {\mathcal {Z}}} can be defined using the correspondence with points on {(1,y)y>0}{\displaystyle {\bigl \{}(1,y)\mid y>0{\bigr \}}} and logarithmic measure on this ray. In consequence, the upper half-plane becomes a metric space. The generic name of this metric space is the hyperbolic plane. In terms of the models of hyperbolic geometry, this model is frequently designated the Poincaré half-plane model.

Complex plane

Mathematicians sometimes identify the Cartesian plane with the complex plane, and then the upper half-plane corresponds to the set of complex numbers with positive imaginary part:

H:={x+iyy>0; x,yR}.{\displaystyle {\mathcal {H}}:=\{x+iy\mid y>0;\ x,y\in \mathbb {R} \}.}

The term arises from a common visualization of the complex number x+iy{\displaystyle x+iy} as the point (x,y){\displaystyle (x,y)} in the plane endowed with Cartesian coordinates. When the y{\displaystyle y} axis is oriented vertically, the "upper half-plane" corresponds to the region above the x{\displaystyle x} axis and thus complex numbers for which y>0{\displaystyle y>0}.

It is the domain of many functions of interest in complex analysis, especially modular forms. The lower half-plane, defined by y<0{\displaystyle y<0} is equally good, but less used by convention. The open unit diskD{\displaystyle {\mathcal {D}}} (the set of all complex numbers of absolute value less than one) is equivalent by a conformal mapping to H{\displaystyle {\mathcal {H}}} (see "Poincaré metric"), meaning that it is usually possible to pass between H{\displaystyle {\mathcal {H}}} and D.{\displaystyle {\mathcal {D}}.}

It also plays an important role in hyperbolic geometry, where the Poincaré half-plane model provides a way of examining hyperbolic motions. The Poincaré metric provides a hyperbolic metric on the space.

The uniformization theorem for surfaces states that the upper half-plane is the universal covering space of surfaces with constant negative Gaussian curvature.

The closed upper half-plane is the union of the upper half-plane and the real axis. It is the closure of the upper half-plane.

Generalizations

One natural generalization in differential geometry is hyperbolic n{\displaystyle n}-spaceHn,{\displaystyle {\mathcal {H}}^{n},} the maximally symmetric, simply connected, n{\displaystyle n}-dimensional Riemannian manifold with constant sectional curvature1{\displaystyle -1}. In this terminology, the upper half-plane is H2{\displaystyle {\mathcal {H}}^{2}} since it has realdimension2.{\displaystyle 2.}

In number theory, the theory of Hilbert modular forms is concerned with the study of certain functions on the direct product Hn{\displaystyle {\mathcal {H}}^{n}} of n{\displaystyle n} copies of the upper half-plane. Yet another space interesting to number theorists is the Siegel upper half-spaceHn,{\displaystyle {\mathcal {H}}_{n},} which is the domain of Siegel modular forms.

See also

References