Suggested 2022-09-19 by Charles Karney
Let and with . Then
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with Cauchy principal value
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Equations (19.25.9)–(19.25.11) correspond to three (nonzero) choices for the last variable of ; see (19.21.7). All terms on the right-hand sides are nonnegative when , , or , respectively.
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If , then the Cauchy principal value is
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The transformations in §19.7(ii) result from the symmetry and homogeneity of functions on the right-hand sides of (19.25.5), (19.25.7), and (19.25.14). For example, if we write (19.25.5) as
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with
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then the five nontrivial permutations of that leave invariant change () into , , , , , and () into , , , , . Thus the five permutations induce five transformations of Legendre’s integrals (and also of the Jacobian elliptic functions).
Let . Then
Assume , , and . Let
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with . Then
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For relations of symmetric integrals to theta functions, see §20.9(i).
With and any permutation of the letters , define
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which implies
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If , then
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compare (19.25.35) and (20.9.3).
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where we assume if , , or ; if , , or ; real if or ; if ; if ; if ; if .
For the use of -functions with in unifying other properties of Jacobian elliptic functions, see Carlson (2004, 2006a, 2006b, 2008).
Inversions of 12 elliptic integrals of the first kind, producing the 12 Jacobian elliptic functions, are combined and simplified by using the properties of . See (19.29.19), Carlson (2005), and (22.15.11), and compare with Abramowitz and Stegun (1964, (17.4.41)–(17.4.52)). For analogous integrals of the second kind, which are not invertible in terms of single-valued functions, see (19.29.20) and (19.29.21) and compare with Gradshteyn and Ryzhik (2015, §3.153,1–10 and §3.156,1–9).
Suggested 2018-03-13 by Felix Ospald
For the notation see §23.2 and §23.3. Let be a lattice for the Weierstrass elliptic function . Then
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for some , provided that satisfies
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The sign on the right-hand side of (19.25.35) will change whenever one crosses a curve on which , for some . Also,
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in which the sign and the are the same as in (19.25.35).
In (19.25.38) and (19.25.39) , , is any permutation of the numbers .
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for some and .
Lastly,
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for some , where
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in which and are generators for the lattice , , and (see (23.2.12)). The sign on the right-hand side of (19.25.40) will change whenever one crosses a curve on which , for some .
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For these results and extensions to the Appell function (§16.13) and Lauricella’s function see Carlson (1963). ( and are equivalent to the -function of 3 and variables, respectively, but lack full symmetry.)