22.12 Expansions in Other Trigonometric Series and Doubly-Infinite Partial Fractions: Eisenstein Series22.14 Integrals

§22.13 Derivatives and Differential Equations

Contents

§22.13(i) Derivatives

Note that each derivative in Table 22.13.1 is a constant multiple of the product of the corresponding copolar functions. (The modulus k is suppressed throughout the table.)

For alternative, and symmetric, formulations of these results see Carlson (2004, 2006a).

§22.13(ii) First-Order Differential Equations

22.13.4 \left(\frac{d}{dz}\mathop{\mathrm{cd}\/}\nolimits\left(z,k\right)\right)^{2}=\left(1-{\mathop{\mathrm{cd}\/}\nolimits^{{2}}}\left(z,k\right)\right)\left(1-k^{2}{\mathop{\mathrm{cd}\/}\nolimits^{{2}}}\left(z,k\right)\right),
22.13.5 \left(\frac{d}{dz}\mathop{\mathrm{sd}\/}\nolimits\left(z,k\right)\right)^{2}={\left(1-{k^{{\prime}}}^{2}{\mathop{\mathrm{sd}\/}\nolimits^{{2}}}\left(z,k\right)\right)}{\left(1+k^{2}{\mathop{\mathrm{sd}\/}\nolimits^{{2}}}\left(z,k\right)\right)},
22.13.6 \left(\frac{d}{dz}\mathop{\mathrm{nd}\/}\nolimits\left(z,k\right)\right)^{2}=\left({\mathop{\mathrm{nd}\/}\nolimits^{{2}}}\left(z,k\right)-1\right)\left(1-{k^{{\prime}}}^{2}{\mathop{\mathrm{nd}\/}\nolimits^{{2}}}\left(z,k\right)\right),
22.13.7 \left(\frac{d}{dz}\mathop{\mathrm{dc}\/}\nolimits\left(z,k\right)\right)^{2}=\left({\mathop{\mathrm{dc}\/}\nolimits^{{2}}}\left(z,k\right)-1\right)\left({\mathop{\mathrm{dc}\/}\nolimits^{{2}}}\left(z,k\right)-k^{2}\right),
22.13.8 \left(\frac{d}{dz}\mathop{\mathrm{nc}\/}\nolimits\left(z,k\right)\right)^{2}={\left(k^{2}+{k^{{\prime}}}^{2}{\mathop{\mathrm{nc}\/}\nolimits^{{2}}}\left(z,k\right)\right)}{\left({\mathop{\mathrm{nc}\/}\nolimits^{{2}}}\left(z,k\right)-1\right)},
22.13.9 \left(\frac{d}{dz}\mathop{\mathrm{sc}\/}\nolimits\left(z,k\right)\right)^{2}=\left(1+{\mathop{\mathrm{sc}\/}\nolimits^{{2}}}\left(z,k\right)\right)\left(1+{k^{{\prime}}}^{2}{\mathop{\mathrm{sc}\/}\nolimits^{{2}}}\left(z,k\right)\right),
22.13.10 \left(\frac{d}{dz}\mathop{\mathrm{ns}\/}\nolimits\left(z,k\right)\right)^{2}=\left({\mathop{\mathrm{ns}\/}\nolimits^{{2}}}\left(z,k\right)-k^{2}\right)\left({\mathop{\mathrm{ns}\/}\nolimits^{{2}}}\left(z,k\right)-1\right),
22.13.11 \left(\frac{d}{dz}\mathop{\mathrm{ds}\/}\nolimits\left(z,k\right)\right)^{2}=\left({\mathop{\mathrm{ds}\/}\nolimits^{{2}}}\left(z,k\right)-{k^{{\prime}}}^{2}\right)\left(k^{2}+{\mathop{\mathrm{ds}\/}\nolimits^{{2}}}\left(z,k\right)\right),
22.13.12 \left(\frac{d}{dz}\mathop{\mathrm{cs}\/}\nolimits\left(z,k\right)\right)^{2}=\left(1+{\mathop{\mathrm{cs}\/}\nolimits^{{2}}}\left(z,k\right)\right)\left({k^{{\prime}}}^{2}+{\mathop{\mathrm{cs}\/}\nolimits^{{2}}}\left(z,k\right)\right).

For alternative, and symmetric, formulations of these results see Carlson (2006a).

§22.13(iii) Second-Order Differential Equations

22.13.16 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{cd}\/}\nolimits\left(z,k\right)=-(1+k^{2})\mathop{\mathrm{cd}\/}\nolimits\left(z,k\right)+2k^{2}{\mathop{\mathrm{cd}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.17 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{sd}\/}\nolimits\left(z,k\right)=(k^{2}-{k^{{\prime}}}^{2})\mathop{\mathrm{sd}\/}\nolimits\left(z,k\right)-2k^{2}{k^{{\prime}}}^{2}{\mathop{\mathrm{sd}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.18 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{nd}\/}\nolimits\left(z,k\right)=(1+{k^{{\prime}}}^{2})\mathop{\mathrm{nd}\/}\nolimits\left(z,k\right)-2{k^{{\prime}}}^{2}{\mathop{\mathrm{nd}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.19 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{dc}\/}\nolimits\left(z,k\right)=-(1+k^{2})\mathop{\mathrm{dc}\/}\nolimits\left(z,k\right)+2{\mathop{\mathrm{dc}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.20 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{nc}\/}\nolimits\left(z,k\right)=(k^{2}-{k^{{\prime}}}^{2})\mathop{\mathrm{nc}\/}\nolimits\left(z,k\right)+2{k^{{\prime}}}^{2}{\mathop{\mathrm{nc}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.21 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{sc}\/}\nolimits\left(z,k\right)=(1+{k^{{\prime}}}^{2})\mathop{\mathrm{sc}\/}\nolimits\left(z,k\right)+2{k^{{\prime}}}^{2}{\mathop{\mathrm{sc}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.22 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{ns}\/}\nolimits\left(z,k\right)=-(1+k^{2})\mathop{\mathrm{ns}\/}\nolimits\left(z,k\right)+2{\mathop{\mathrm{ns}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.23 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{ds}\/}\nolimits\left(z,k\right)=(k^{2}-{k^{{\prime}}}^{2})\mathop{\mathrm{ds}\/}\nolimits\left(z,k\right)+2{\mathop{\mathrm{ds}\/}\nolimits^{{3}}}\left(z,k\right),
22.13.24 \frac{{d}^{2}}{{dz}^{2}}\mathop{\mathrm{cs}\/}\nolimits\left(z,k\right)=(1+{k^{{\prime}}}^{2})\mathop{\mathrm{cs}\/}\nolimits\left(z,k\right)+2{\mathop{\mathrm{cs}\/}\nolimits^{{3}}}\left(z,k\right).

For alternative, and symmetric, formulations of these results see Carlson (2006a).