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Theory and Modern Applications

Table 1 Jacobi elliptic functions

From: Exact spatiotemporal soliton solutions to the generalized three-dimensional nonlinear Schrödinger equation in optical fiber communication

Solution

\(\boldsymbol{q_{2}}\)

\(\boldsymbol{q_{4}}\)

F

1

\(-(1+M^{2})\)

\(M^{2}\)

sn

2

\(2M^{2}-1\)

\(-M^{2}\)

cn

3

\(2-M^{2}\)

−1

dn

4

\(-(1+M^{2})\)

1

ns

5

\(2M^{2}-1\)

\(1-M^{2}\)

nc

6

\(2-M^{2}\)

\(M^{2}-1\)

nd

7

\(2-M^{2}\)

\(1-M^{2}\)

sc

8

\(2M^{2}-1\)

\(-M^{2}(1-M^{2})\)

sd

9

\(2-M^{2}\)

1

cs

10

\(-(1+M^{2})\)

\(M^{2}\)

cd

11

\(2M^{2}-1\)

1

ds

12

\(-(1+M^{2})\)

1

dc

13

\(M^{2}/2-1\)

\(M^{4}/4\)

sn/(1 + dn)

14

\(M^{2}/2-1\)

\(M^{4}/4\)

\(\mathrm{cn}/(\sqrt{1-M^{2}}+\mathrm{dn})\)