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[24
24.
ON THE INVERSE ELLIPTIC FUNCTIONS.
[From the Cambridge Mathematical Journal, t. iv. (1845), pp. 257—277.]
The properties of the inverse elliptic functions have been the object of the
researches of the two illustrious analysts, Abel and Jacobi. Among their most remarkable
ones may be reckoned the formulae given by Abel (Œuvres, t. I. p. 212 [Ed. 2, p. 343]), in
which the functions cf>a, fa, Fa, (corresponding to J acobi’s sin am . a, cos am . a, A am . a,
though not precisely equivalent to these, Abel’s radical being [(1 — tfx-) (1 + e 2 # 2 )]*, and
Jacobi’s, like that of Legendre’s [(1 — x 2 ) (1 — k^xf]^), are expressed in the form of fractions,
having a common denominator ; and this, together with the three numerators, resolved
into a doubly infinite series of factors ; i.e. the general factor contains two independent
integers. These formulae may conveniently be referred to as “ Abel’s double factorial
expressions” for the functions <£, f F. By dividing each of these products into an
infinite number of partial products, and expressing these by means of circular or
exponential functions, Abel has obtained (pp. 216—218) two other systems of formulae for
the same quantities, which may be referred to as “Abel’s first and second single factorial
systems.” The theory of the functions forming the above numerators and denominator,
is mentioned by Abel in a letter to Legendre (Œuvres, t. II. p. 259 [Ed. 2, p. 272]), as
a subject to which his attention had been directed, but none of his researches upon
them have ever been published. Abel’s double factorial expressions have nowhere any
thing analogous to them in Jacobi’s Fund. Nova; but the system of formulae analogous
to the first single factorial system is given by Jacobi (p. 86), and the second system
is implicitly contained in some of the subsequent formulae. The functions forming the
numerator and denominator of sin am. u, Jacobi represents, omitting a constant factor,
by H (u), © (u) ; and proceeds to investigate the properties of these new functions. This
he principally effects by means of a very remarkable equation of the form
/© ( w ) = 1/1 y? + BJ 0 du. f 0 du sin 2 am u,