Mathematics

Weierstrass’s Al Functions

1

To the system of equations relating integrals ["Integralgleichungen"] from which, according to Jacobi, one must begin in the theory of Abelian integrals ["Abelsche funktionen"], I shall give the following form, which I have recognized to be the simplest and most appropriate one. Let

be a polynomial function of degree

here I assume to begin with that the quantities
are all real and ordered in such a way that

Now let R(x) be decomposed into two factors,

and

Considering

as independent variables and
as functions of them, let the relations between these 2n variables be expressed by the following n equations:

With the help of Abel’s Theorem, I now establish in detail the proposition already stated by Jacobi, which I consider the foundation of the whole theory, namely, that whereas for given values of

the quantities
have infinitely many different values, if, conversely,
are given, then the values of
as well as the corresponding values of
are uniquely determined. Moreover . . .
are the roots of a [polynomial] equation of degree n whose coefficients are . . . single-valued functions of the independent variables
while a second polynomial function of x, whose coefficients are the same kind of functions of
gives for
the corresponding values of

Therefore, every symmetric rational function of

can be regarded as a single-valued function of
In particular, it becomes evident that

where a signifies one of the integers

is the square of such a function. Accordingly, I denote by
the largest integer less than or equal to a/2 and set

I also denote

and call the

quantities
etc., Abelian functions, since they are the ones which completely correspond to the elliptic functions2 sn u, cn u, dn u. The series, expanded in powers of
have the following form:

In these formulas j stands for any one of the integers

k for any of the integers
and
designates a homogeneous polynomial of degree α. I note generally that j and l as well as j′ and l′ will stand below for one of the integers
k, on the other hand, will stand for one of the integers
It is to be noted further that wherever there appears the root (of 2nd or 4th degree) of a positive expression, formed by multiplication and division of the differences
etc., its positive value shall always be taken.

. . . . .

2.

Now I shall introduce those quantities which are analogous to the so-called complete elliptic integrals of the first kind. If x is real and lies between the limits

and aα, then

and hence one can set

where all roots are to be taken as positive.

Furthermore, if x lies between + ∞ and a0,

and if x lies between a2n and – ∞:

Now if a and b are two real quantities, and F(x) denotes a rational function of x, then I designate by

that particular value of the integral

which is obtained if in the integration
is always determined by the above formulas, using the upper [positive] sign. Assuming this, let

be designated by

Then the relation

for

holds.

Further, let

so that

where

is to be taken as positive in the first integration,
in the other one. Then it turns out that

A special case of Abel’s Theorem then leads to the following formulas, in which α, β, γ denote numbers from the set

and the symbol
denotes 0 when
and 1 when

From this, one may deduce

and if one sets

where

represent arbitrary integers, then

Now set

and

where

also designate arbitrary integers; one obtains the formulas

where, if

, m0 must be taken equal to zero; and

in which formula the factor of

is to be set equal to 1 for
With the help of formula (17), one obtains similar relations for the functions

The functions

have the peculiar property ["Eigenthümlichkeit"] that they all have the same singularities ["für dieselben Betrâgen der
unendlich werden"]. Furthermore, as will be shown in the proof of the main theorem given in §1 (if one specifies fixed limits, arbitrarily large, for the absolute values of
which they are not to exceed), each of the mcan be represented as the quotient of two series, expanded in positive integral powers of
which converge for all values of these variables within the assigned limits. This leads to the conjecture that
might be represented as fractions with a common denominator, in which this denominator as well as the numerators would be functions of
which would never become infinite, and could be expanded in uniformly convergent series of integral positive powers of their arguments. If
(where p and pα are functions of the type just described), then d log Al(u1 , . . .) mustconsist of two parts, one of which becomes infinite for all values of
for which
the other, for all those values which cause
to become infinite. The same is the case for the higher logarithmic differentials of
Let us assume now that

where

when
then one can set du log
and, since Pα, P can be expressed in terms of
hence also in terms of
one must arrive in this way at
differential equations for the
quantities indicated.

For elliptic functions, the calculation is very easy. For, if

one has:

Now if one sets

there results

This equation can be factored, giving the two equivalent equations

It has been shown previously that, if the absolute value of u has an upper bound M, sn u can be represented as the quotient of two series of integral powers of u, converging for all values of the variable less than M; hence it can be proved rigorously that the two functions p and p1 defined by the two preceding differential equations can be expanded into uniformly convergent (for all real and imaginary values of u) series of positive integral powers of u. And if the four arbitrary constants which they contain are determined so that, for

then, indeed,

There are similar expansions for cn u, dn u, and in this way one arrives at those representations of elliptic functions which Abel had mentioned in a letter to Legendre3 without giving the details, or any indication of the procedure. From the functions p and p1 one also obtains the Jacobian functions

Θ(u) and H(u) easily, and thus can carry out the development of elliptic functions in all forms without basing them on transformation or multiplication formulas. The above differential equations for p and p1 can be made a basis for the complete theory of elliptic transcendental functions.

1 K. Weierstrass "Zur Theorie der Abelsche Funktionen," J. reine ang. Math. 52 (1856), 285–339; Werke, I, 297–355.

2 Like Jacobi, Weierstrass wrote sin am u, cos am u, Δ am u where we have written sn u, cn u, and dn u.

3 See J. reine ang. Math., vol. 4, p. 244; also vol. 6, p. 76 (K. W.)