Math 2.0

Special functions Elliptic integrals and elliptic functions Theorem

Addition formulas for Jacobi elliptic functions

Builds on Jacobi elliptic functions

Statement

Let 0<k<10 < k < 1, and let sn⁡\operatorname{sn}, cn⁡\operatorname{cn}, dn⁡\operatorname{dn} be the Jacobi elliptic functions with modulus kk. For all complex u,vu, v such that both sides are defined, with Δ=1−k2sn⁡2usn⁡2v,\Delta = 1 - k^2\operatorname{sn}^2 u \operatorname{sn}^2 v, one has sn⁡(u+v)=sn⁡ucn⁡vdn⁡v+sn⁡vcn⁡udn⁡uΔ,\operatorname{sn}(u + v) = \frac{\operatorname{sn} u \operatorname{cn} v \operatorname{dn} v + \operatorname{sn} v \operatorname{cn} u \operatorname{dn} u}{\Delta}, cn⁡(u+v)=cn⁡ucn⁡v−sn⁡usn⁡vdn⁡udn⁡vΔ,\operatorname{cn}(u + v) = \frac{\operatorname{cn} u \operatorname{cn} v - \operatorname{sn} u \operatorname{sn} v \operatorname{dn} u \operatorname{dn} v}{\Delta}, dn⁡(u+v)=dn⁡udn⁡v−k2sn⁡usn⁡vcn⁡ucn⁡vΔ.\operatorname{dn}(u + v) = \frac{\operatorname{dn} u \operatorname{dn} v - k^2 \operatorname{sn} u \operatorname{sn} v \operatorname{cn} u \operatorname{cn} v}{\Delta}.

Remarks

Proof idea: fix cc and set v=c−uv = c - u; using the derivative rules sn⁡′=cn⁡dn⁡\operatorname{sn}' = \operatorname{cn}\operatorname{dn}, cn⁡′=−sn⁡dn⁡\operatorname{cn}' = -\operatorname{sn}\operatorname{dn}, dn⁡′=−k2sn⁡cn⁡\operatorname{dn}' = -k^2\operatorname{sn}\operatorname{cn} and the relations sn⁡2+cn⁡2=1\operatorname{sn}^2 + \operatorname{cn}^2 = 1, dn⁡2+k2sn⁡2=1\operatorname{dn}^2 + k^2\operatorname{sn}^2 = 1, one checks that each right side has derivative 00 in uu. So each right side depends only on u+v=cu + v = c, and putting u=0u = 0 (where sn⁡0=0\operatorname{sn} 0 = 0, cn⁡0=dn⁡0=1\operatorname{cn} 0 = \operatorname{dn} 0 = 1) shows it equals the left side. By analytic continuation the identities hold wherever both sides are defined. Example: for k→0k \to 0 the formulas become sin⁡(u+v)=sin⁡ucos⁡v+sin⁡vcos⁡u\sin(u + v) = \sin u\cos v + \sin v\cos u and the cosine addition formula, with dn⁡=1\operatorname{dn} = 1 and Δ=1\Delta = 1. With k=1k = 1, where sn⁡=tanh⁡\operatorname{sn} = \tanh and cn⁡=dn⁡=sech⁡\operatorname{cn} = \operatorname{dn} = \operatorname{sech}, the first formula becomes tanh⁡(u+v)=(tanh⁡u+tanh⁡v)/(1+tanh⁡utanh⁡v)\tanh(u + v) = (\tanh u + \tanh v)/(1 + \tanh u\tanh v), after factoring 1−tanh⁡2utanh⁡2v=(1−tanh⁡utanh⁡v)(1+tanh⁡utanh⁡v)1 - \tanh^2 u\tanh^2 v = (1 - \tanh u\tanh v)(1 + \tanh u\tanh v). Example of use: with v=Kv = K, where sn⁡K=1\operatorname{sn} K = 1, cn⁡K=0\operatorname{cn} K = 0, dn⁡K=k′\operatorname{dn} K = k', one gets sn⁡(u+K)=cn⁡u/dn⁡u\operatorname{sn}(u + K) = \operatorname{cn} u / \operatorname{dn} u.

Going deeper

For a student

The addition formulas reflect the group law on the elliptic curve y2=(1−x2)(1−k2x2)y^2 = (1 - x^2)(1 - k^2x^2), parametrised by x=sn⁡ux = \operatorname{sn} u, y=cn⁡udn⁡uy = \operatorname{cn} u\operatorname{dn} u. They give the shifts by quarter and half periods, such as sn⁡(u+2K)=−sn⁡u\operatorname{sn}(u + 2K) = -\operatorname{sn} u, from the special values at KK and 2K2K. They are also the algebraic addition theorem behind Euler's addition theorem for the integral ∫dt/(1−t2)(1−k2t2)\int dt/\sqrt{(1 - t^2)(1 - k^2t^2)}.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Jacobi_elliptic_functions
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