An Introduction to the Theory of Multiply Periodic Functions

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(ii) When / is an elementary integral of the third kind, that is, is infinite at one place (a) like log 4, where t^ is the parameter for this place, and infinite at another place (/3) like — log fp, but not elsewhere, we have, whatever Z may be ij|^^;ij(..,^)cfe=iog|g, where Z{a), Z(^) denote the values of Z at these places, (iii) If the fundamental algebraic equation be y^-(4!x'-g.^x-gs) = 0, and R (x, y) = x/y, while Z is taken to be (y — mx — c)/(y — m^x — Co), we have Q = 3, and dljdt is in
...finite only for ^ = oo ; putting, for the single place there occurring, x = t-\ y = -2t-'(l-ig,t'-...), we have f^=la-y,t' -...), 1 y — mx — c , 1 4- ^mt + \ct^ - ... ^ , , , log -^ = log = ^r^-- T— TT- = i (m - ?Wo) t + ..
^y-nioX-Co ^ l+lniot + Uot'- ... ^^ ^ NOTE ii] Converse of Abel's Theorem. 181 and ■(f) ■»^^" t-^ \ {m - mo); if then (^i, 3/1), (x^, 3/2) and (^3, 3/3) be the three intersections of the straight line y — mx-\- c with the cubic curve y- = ^x^ — g^x — g^, and (ci), {c^, (Ca) be arbitrary places, we have r(*^') xdx A*^) xdx A^3) xdx ^yi — y^ /-i ■ hej y he.) y he,) y ^^x,-x,~ ' where is a quantity unaltered by replacing the straight line y = mx + c by any other ; putting, as usual ^ y this is equivalent with r°° dx 1 r*' r 1 du, till) -\-K(v)-t(u-\-v)-irl ^ — ^ = constant, for arbitrary values of il and v ; by expansion in powers of u for small values of u we at once find the constant to be zero.


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