Digital Library of Mathematical Functions
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22 Jacobian Elliptic FunctionsProperties

§22.11 Fourier and Hyperbolic Series

Throughout this section q and \zeta are defined as in §22.2.

If q\mathop{\exp\/}\nolimits\!\left(2|\imagpart{\zeta}|\right)<1, then

Next, if q\mathop{\exp\/}\nolimits\!\left(|\imagpart{\zeta}|\right)<1, then

In (22.11.7)–(22.11.12) the left-hand sides are replaced by their limiting values at the poles of the Jacobian functions.

Next, with \mathop{E\/}\nolimits=\mathop{E\/}\nolimits\!\left(k\right) denoting the complete elliptic integral of the second kind (§19.2(ii)) and q\mathop{\exp\/}\nolimits\!\left(2|\imagpart{\zeta}|\right)<1,

Similar expansions for {\mathop{\mathrm{cn}\/}\nolimits^{{2}}}\left(z,k\right) and {\mathop{\mathrm{dn}\/}\nolimits^{{2}}}\left(z,k\right) follow immediately from (22.6.1).

For further Fourier series see Oberhettinger (1973, pp. 23–27).