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RePoSS #11: The Mathematics of Niels Henrik Abel: Continuation ...

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18.1. Transformation theory 333<br />

<strong>The</strong> central question <strong>of</strong> transformation theory. ABEL picked up the theme <strong>of</strong> trans-<br />

formations <strong>of</strong> elliptic integrals from LEGENDRE. In ABEL’S words, the central problem<br />

was posed with variations on multiple occasions, for instance in the following way:<br />

“To find all the possible cases in which one can satisfy the differential equation<br />

dy<br />

�<br />

(1 − y2 ) � 1 − c2 = a<br />

1y2� dx<br />

� (1 − x 2 ) (1 − c 2 x 2 )<br />

by an algebraic equation between the variables x and y and supposing the moduli c<br />

and c1 less than unity and the coefficient a either real or imaginary.” 6<br />

Expressed in the notation <strong>of</strong> LEGENDRE’S differentials, the above question asks<br />

for every possible way <strong>of</strong> transforming x algebraically into y in such a way that the<br />

integral with modulus c1 transformed into the integral with modulus c.<br />

18.1.1 ABEL’s response to JACOBI’s announcements<br />

ABEL first published in the Astronomische Nachrichten in 1828; 7 in a lengthy paper, he<br />

demonstrated how the theory which he had developed in his Recherches could answer<br />

a question raised by JACOBI. In the paper — which is entitled Solution d’un problème<br />

général concernant la transformation des fonctions elliptiques — , 8 ABEL began by describ-<br />

ing key results concerning the inverse <strong>of</strong> elliptic integrals deduced in the Recherches.<br />

With the notation<br />

and the inversion<br />

∆ (x) =<br />

�<br />

θ =<br />

0<br />

�<br />

(1 − c 2 x 2 ) (1 − e 2 x 2 )<br />

dx<br />

and x = λ (θ) ,<br />

∆ (x)<br />

ABEL presented the highlights <strong>of</strong> the Recherches in two theorems which summarize<br />

(16.3) and (16.8), respectively. First, he expressed the addition theorem for the elliptic<br />

function <strong>of</strong> the first kind λ,<br />

λ � θ ± θ ′� = λ (θ) ∆ (θ′ ) ± λ (θ ′ ) ∆ (θ)<br />

1 − c2e2λ2 (θ) λ2 (θ ′ .<br />

)<br />

Second, ABEL described the conditions on the arguments which ensured that the func-<br />

tion took identical values,<br />

λ (θ) = λ � θ ′� if and only if θ ′ = (−1) m+m′<br />

θ + mω + m ′ ω ′<br />

6 “Trouver tous les cas possibles où l’on pourra satisfaire à l’équation différentielle:<br />

dy<br />

�<br />

(1 − y2 ) � 1 − c2 = a<br />

1y2� dx<br />

� (1 − x 2 ) (1 − c 2 x 2 )<br />

(18.1)<br />

par une équation algébrique entre les variables x et y, en supposant les modules c et c1 moindre que<br />

l’unité et le coeffcient a réel ou imaginaire.” (N. H. <strong>Abel</strong>, 1829a, 33).<br />

7 (N. H. <strong>Abel</strong>, 1828d). <strong>The</strong> paper is dated 27 May 1828.<br />

8 (ibid.).

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