Hyperbolic geometry – more parallels

Posted on 2017/04/09 by arkajad

Non-Euclidean geometry was invented because not everybody was happy with the fifth postulate of plane Euclid’s geometry. The fifth postulate can be formulated in several equivalent ways, one of its versions, the one that is of interest for us, states that for every straight line and every point that is not on this line, there is a unique parallel line passing through this point. The definition of parallel lines is that they extend infinitely long in both direction without intersection.

Many mathematicians believed that the fifth postulate should somehow follow from other postulates – until models of geometry were constructed with all other postulates satisfied, but the fifth postulate violated. Hyperbolic geometry of the disk that we are studying has this property.

We started playing with parallel lines of the disk geometry in the last post. We will continue it now, but, for change, we will play a little bit more with the devil of the algebra.

Our hyperbolic geometry model is based on invariants of the fractional linear action of SU(1,1) on the unit disk D in the complex plane. The group SU(1,1) acts transitively on the disk. In SU(1,1) decomposition we have seen that every matrix A in SU(1,1) can be uniquely decomposed into a product A=P(z)U(\theta), with P(z),\, z\in D, positive and U(\theta) unitary, both in SU(1,1).

(1)   \begin{equation*} P(z)=\frac{1}{\sqrt{1-|z|^2}}\begin{bmatrix}1&\bar{z}\\ z&1\end{bmatrix},\end{equation*}

(2)   \begin{equation*}U(\theta)=\begin{bmatrix}e^{i\theta}&0\\0&e^{-i\theta}\end{bmatrix}.\end{equation*}

The fractional linear transformation defined by P(z) maps the origin 0\in D to z.

Remark: Given a complex 2\times 2 matrix A=\left(\begin{smallmatrix}\lambda&\mu\\ \nu&\rho\end{smallmatrix}\right) we define its action on the complex plane by the fractional linear transformation

(3)   \begin{equation*} A:z\mapsto \frac{\rho z+\nu}{\mu z+\lambda}.\end{equation*}

This is our choice. Another possible choice, that is often used, would be (\lambda z+\mu)/(\nu z+\rho).

The matrix P(z) is positive, but positivity is not an intrinsic (or “natural”) property within SU(1,1). If S is in SU(1,1), then the matrix SP(z)S^{-1} is “similar” to P(z), but it is not necessarily positive. While it also has positive eigenvalues, it is not necessarily Hermitian. Intrinsic, natural, properties should be invariant under similarity transformations. Therefore, if only for esthetic reasons, for beauty and for pleasure, we will take now a different road. Within the group SU(1,1) there are special matrices known as parabolic. Parabolic matrices are characterized by the property that they have trace equal 2. This property is invariant under similarity transformations. Our matrix P(z) has trace different from 2. But we can compensate it by multiplying from the right by a unitary matrix, and that is what we will do now.

Multiplying P(z) with U(\theta) from the right we get

(4)   \begin{equation*}P(z)U(\theta)=\frac{1}{\sqrt{1-|z|^2}}\begin{bmatrix}e^{i\theta}&\bar{z}e^{-i\theta}\\ ze^{i\theta}&e^{-i\theta}\end{bmatrix}.\end{equation*}

If we want to obtain trace equal 2, we should have

(5)   \begin{equation*}\cos \theta=\sqrt{1-|z|^2}.\end{equation*}

If \cos \theta=\sqrt{1-|z|^2}, then for \sin \theta we have two possibilities:

(6)   \begin{equation*}\sin \theta=\pm|z|.\end{equation*}

Let us choose the first possibility. Then e^{i\theta}=\sqrt{1-|z|^2}+i|z|,\, e^{-i\theta}=\sqrt{1-|z|^2}-i|z|.

We define, for each z in the disk, the matrix Q(z) as

(7)   \begin{equation*}Q(z)=P(z)U(\theta)= \begin{bmatrix}1+\frac{i|z|}{\sqrt{1-|z|^2}}&\bar{z}(1-\frac{i|z|}{\sqrt{1-|z|^2}})\\ z(1+\frac{i|z|}{\sqrt{1-|z|^2}})&1-\frac{i|z|}{\sqrt{1-|z|^2}}\end{bmatrix}.\end{equation*}

With this definition Q(z) maps 0 to z as before, but now Q(z) is parabolic.

In Hyperbolic geometry – Playing with parallels we were constructing SU(1,1) transformations that were mapping the straight line on the real axis on the disk into parallel lines that were limiting parallel lines – they asymptotically converged to the points z=-1 or z=1 on the unit circle – the boundary of the disk:

Template and two limiting parallels

Here I will do the same, but using a different method, with parabolic transformations. The advantage will be that all will be clean algebraic, no hyperbolic or trigonometric functions will be needed. The devil of the algebra will be collaborating with the angel of geometry in one common project.

Let us find Q(z) that leave the point z=1 fixed. Using Eqs. (3 and (7) we obtain

(8)   \begin{equation*}1-\frac{i|z|}{\sqrt{1-|z|^2}}+z(1+\frac{i|z|}{\sqrt{1-|z|^2}})=\bar{z}(1-\frac{i|z|}{\sqrt{1-|z|^2}})+1+\frac{i|z|}{\sqrt{1-|z|^2}}.\end{equation*}

Writing z=x+iy, after some simple manipulations, we obtain a particular solution (I am using Mathematica for such tasks):

    \[ y=\sqrt{x-x^2},\]

which makes sense 0\leq x<1. Substituting this expression in the formula for Q(z) produces a family Q_1(x) parametrized by x

    \[Q_1(x)=Q(x+i\sqrt{x-x^2})=\begin{bmatrix} \frac{i \sqrt{x}}{\sqrt{1-x}}+1 & \frac{\left(\sqrt{1-x}-i \sqrt{x}\right) \left(x-i \sqrt{-(x-1) x}\right)}{\sqrt{1-x}} \\ \frac{\left(\sqrt{1-x}+i \sqrt{x}\right) \left(x+i \sqrt{-(x-1) x}\right)}{\sqrt{1-x}} & 1-\frac{i \sqrt{x}}{\sqrt{1-x}} \end{bmatrix}.\]

The form suggests introducing a new variable, t=\sqrt{x}/\sqrt{1-x}. Then the formula simplifies dramatically:

(9)   \begin{equation*}Q_1(t)=\begin{bmatrix} 1+i t & -i t \\ i t & 1-i t \end{bmatrix}.\end{equation*}

This way we have obtained a very simple family of parabolic transformations, each of them having the point z=1 fixed. Below is the result of applying these transformations to the straight line along the real axis for t=\pm 2^s, with s in the range (-2,2), step 0.1.

Hyperbolic geometry right asymptotic parallels

The family Q_1(t) is, in fact, a one-parameter group of parabolic elements in SU(1,1). We have Q_1(t)Q_1(s)=Q_1(t+s), and
Q_1(t)=\exp tY_1, where

(10)   \begin{equation*}Y_1=\begin{bmatrix}i& -i\\i& -i\end{bmatrix}.\end{equation*}

The matrix Y_1 has the “nilpotent” property Y_1^2=0, therefore \exp tY_1 reduces to \exp tY_1=I+tY_1.

Repeating the same as above, but for z=-1 we would get one-parameter group of parabolic matrices Q_{-1}(t)

(11)   \begin{equation*}Q_1(t)=\exp t Y_{-1}=\begin{bmatrix} 1-i t & -i t \\ i t & 1+i t\end{bmatrix},\quad Y_{-1}=\begin{bmatrix}-i&-i\\i&i\end{bmatrix}\end{equation*}

Hyperbolic geometry left and right asymptotic parallels

Let us now return to the transformations Q_1(t) and how they transform the points on the real axis into a segment of a circle – circle according to the Euclidean geometry, straight line according to hyperbolic geometry. Using Eqs. (9) and (3) we get:

(12)   \begin{equation*}Q_1(t):x\mapsto \frac{(1-i t) x+i t}{-i t x+i t+1}=\frac{t^2 (x-1)^2 + x +i(t (x-1)^2)}{1 + t^2 (x-1)^2}.\end{equation*}

Let us take one particular line, say, for t=0.4. WE easily find that the real part of the expression above vanishes at x=-1/4. the imaginary part at this point is y=1/2. Thus the line defined by t=0.4 transformation intersects the vertical imaginary axis at the point p with y=1/2. The same holds for the line defined by Q_{-1}(0.4).

We now want to find the formula for all lines parallel to the real axis and crossing the point p. So far we know two of them – the limiting lines:

Hyperbolic geometry left and right limiting parallels

First: how to draw all straight lines passing through p? Simple: we draw straight lines through the origin z=0, which is easy. Then we shift it to the point p using either P(z_0) or Q(z_0) with z_0=0.5i.

Here we can see the difference between shifts of straight lines implemented by the parabolic operation Q(z_0) and the positive operation P(z_0).

The red line is the shift of real axis by P(z_0) The white line is the shift by Q(z_0). The red line crosses the vertical line, joining o and p, at right angle, in a left-right symmetric way. The white line, on the other hand, crosses the horizontal and the vertical line at the same angle. I did not try to prove it, but it seems from the graph that this is the case. If so, then a proof should be straightforward, and Q(z) could be useful for creating hyperbolic squares and demonstrating that the larger is the square, the smaller is the sum of its four angles.

For our present purpose of creating a family of straight lines through p, and parallel to the real axis, it is more convenient to use P(z_0)

(13)   \begin{equation*}P(z_0)=\frac{1}{\sqrt{3}}\begin{bmatrix}2&-i\\i&2\end{bmatrix}.\end{equation*}

Given angle \phi, 0\leq\phi\leq \pi the line through the origin is re^{i\phi} where r varies between -1 and 1. We lift it using P(z_0) and get

(14)   \begin{equation*}z(r)=\frac{2re^{i\phi}+i}{-ire^{i\phi}+2}.\end{equation*}

We look at the left end, for r=-1, and find for which \phi=\phi_0 we have z(-1)=-1. That is easy and the result is

(15)   \begin{equation*}\phi_0=\arctan (4/3)=0.927295.\end{equation*}

In fact, we could obtain this value by examining the angle of intersection of the limiting line with the vertical. I checked it numerically. Geometrical justification is probably easy. Notice that our particular angle happens to be one of the angles of the famous Pythagorean 3-4-5 triangle.

We can now draw a family of straight lines through the origin, with angles between \phi_0 and \phi_0.

Hyperbolic geometry parallel lines through a point

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5 Responses to Hyperbolic geometry – more parallels

  2. Bjab says:
    2017/04/10 at 15:29

    fifth postulated ->
    fifth postulate

    of interests ->
    of interest

    phi and theta mismatched in (2) and sentences above (2)

    different rode ->
    ?

  3. Bjab says:
    2017/04/12 at 13:01

    Eq. (4) lacks z

    the positive operation ->
    and the positive operation

    The red line is the shift ->
    I can’t see any red line

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