The boundary of the rectangle
, with vertices 0,
,
,
, is mapped strictly monotonically by
onto the real line with
,
,
,
,
. There is a
unique point
such
that
. The interior of
is mapped
one-to-one onto the lower half-plane.
The two pairs of edges
and
of
are each
mapped strictly monotonically by
onto the real line, with
,
,
; similarly for the
other pair of edges. For each pair of edges there is a unique point
such
that
.
The interior of the rectangle with vertices 0,
,
,
is mapped two-to-one onto the lower half-plane. The
interior of the rectangle with vertices 0,
,
,
is mapped
one-to-one onto the lower half-plane with a cut from
to
. The cut is the image of
the edge from
to
and is not a line segment.
For examples of conformal mappings of the function
,
see Abramowitz and Stegun (1964, pp. 642–648, 654–655, and 659–60).
For conformal mappings via modular functions see Apostol (1990, §2.7).
An algebraic curve that can be put either into the form
or equivalently, on replacing
by
and
by
(projective
coordinates), into the form
is an example of an elliptic curve (§22.18(iv)).
Here
and
are real or complex constants.
Points
on the curve can be parametrized by
,
, where
and
: in this case we write
. The
curve
is made into an abelian group (Macdonald (1968, Chapter 5))
by defining the zero element
as the
point at infinity, the negative of
by
, and generally
on the curve iff the points
,
,
are collinear. It follows from the addition formula (23.10.1)
that the points
,
, have zero sum iff
, so that addition of points on the curve
corresponds to addition of parameters
on the torus
;
see McKean and Moll (1999, §§2.11, 2.14).
In terms of
the addition law can be expressed
,
; otherwise
, where
and
If
, then
intersects the plane
in a curve that is
connected if
; if
, then the
intersection has two components, one of which is a closed loop. These cases
correspond to rhombic and rectangular lattices, respectively. The addition law
states that to find the sum of two points, take the third intersection with
of the chord joining them (or the tangent if they coincide); then its
reflection in the
-axis gives the required sum. The geometric nature of this
construction is illustrated in McKean and Moll (1999, §2.14),
Koblitz (1993, §§6, 7), and
Silverman and Tate (1992, Chapter 1, §§3, 4): each of these references
makes a connection with the addition theorem (23.10.1).
If
, then by rescaling we may assume
.
Let
denote the set of points on
that are of finite order (that is,
those points
for which there exists a positive integer
with
),
and let
be the sets of points with integer and
rational coordinates, respectively. Then
.
Both
are subgroups of
, though
may not be.
always has the form
(Mordell’s Theorem:
Silverman and Tate (1992, Chapter 3, §5)); the determination of
, the
rank of
, raises questions of
great difficulty, many of which are still open. Both
and
are finite sets.
must have one of the forms
,
or
, or
,
. To determine
, we make use of the fact that if
then
must be a divisor of
; hence there are only a
finite number of possibilities for
. Values of
are then found as integer
solutions of
(in particular
must be a divisor of
). The resulting points are then tested for finite order as follows.
Given
, calculate
,
,
by doubling as above. If any of these
quantities is zero, then the point has finite order. If any of
,
,
is not an integer, then the point has infinite order. Otherwise observe any
equalities between
,
,
,
, and their negatives. The order of a
point (if finite and not already determined) can have only the values
3, 5, 6, 7, 9, 10, or 12, and so can be found from
,
,
,
,
,
, or
. If none of these
equalities hold, then
has infinite order.
For extensive tables of elliptic curves see Cremona (1997, pp. 84–340).
The modular equation of degree
,
prime, is an algebraic equation
in
and
. For
and with
,
, the modular
equation is as follows: