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21: 23.10 Addition Theorems and Other Identities

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23.10.10 $$\sigma \left(2z\right)=-{\mathrm{\wp }}^{\prime }\left(z\right){\sigma }^4\left(z\right).$$

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Symbols:

$\mathrm{\wp }\left(z\right)$ (= $\mathrm{\wp }\left(z|𝕃\right)$ = $\mathrm{\wp }(z;g_2,g_3)$): Weierstrass $\mathrm{\wp }$-function, $\sigma \left(z\right)$ (= $\sigma \left(z|𝕃\right)$ = $\sigma (z;g_2,g_3)$): Weierstrass sigma function, $𝕃$: lattice and $z$: complex

A&S Ref:

18.4.8

Referenced by:

§23.10(ii)

Permalink:

http://dlmf.nist.gov/23.10.E10

Encodings:

pMML, png, TeX

See also:

Annotations for §23.10(ii), §23.10 and Ch.23

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23.10.17 $$\mathrm{\wp }\left(cz|c𝕃\right)=c^{-2}\mathrm{\wp }\left(z|𝕃\right),$$

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Symbols:

$\mathrm{\wp }\left(z\right)$ (= $\mathrm{\wp }\left(z|𝕃\right)$ = $\mathrm{\wp }(z;g_2,g_3)$): Weierstrass $\mathrm{\wp }$-function, $𝕃$: lattice, $z$: complex and $c$: constant

A&S Ref:

18.2.2

Permalink:

http://dlmf.nist.gov/23.10.E17

Encodings:

pMML, png, TeX

See also:

Annotations for §23.10(iv), §23.10 and Ch.23

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23.10.18 $$\zeta \left(cz|c𝕃\right)=c^{-1}\zeta \left(z|𝕃\right),$$

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Symbols:

$\zeta \left(z\right)$ (= $\zeta \left(z|𝕃\right)$ = $\zeta (z;g_2,g_3)$): Weierstrass zeta function, $𝕃$: lattice, $z$: complex and $c$: constant

A&S Ref:

18.2.3

Permalink:

http://dlmf.nist.gov/23.10.E18

Encodings:

pMML, png, TeX

See also:

Annotations for §23.10(iv), §23.10 and Ch.23

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23.10.19 $$\sigma \left(cz|c𝕃\right)=c\sigma \left(z|𝕃\right).$$

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Symbols:

$\sigma \left(z\right)$ (= $\sigma \left(z|𝕃\right)$ = $\sigma (z;g_2,g_3)$): Weierstrass sigma function, $𝕃$: lattice, $z$: complex and $c$: constant

A&S Ref:

18.2.4

Permalink:

http://dlmf.nist.gov/23.10.E19

Encodings:

pMML, png, TeX

See also:

Annotations for §23.10(iv), §23.10 and Ch.23

►Also, when $𝕃$ is replaced by $c𝕃$ the lattice invariants $g_2$ and $g_3$ are divided by $c^4$ and $c^6$, respectively. …

22: 33.24 Tables

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Abramowitz and Stegun (1964, Chapter 14) tabulates $F_0(\eta ,\rho )$, $G_0(\eta ,\rho )$, $F_0^{\prime }(\eta ,\rho )$, and $G_0^{\prime }(\eta ,\rho )$ for $\eta =0.5(.5)20$ and $\rho =1(1)20$, 5S; $C_0\left(\eta \right)$ for $\eta =0(.05)3$, 6S.

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23: 18.36 Miscellaneous Polynomials

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§18.36(v) Non-Classical Laguerre Polynomials $L_n^{(-k)}\left(x\right)$, $k=1,2\mathrm{\dots }$

… ►For the Laguerre polynomials $L_n^{(\alpha )}\left(x\right)$ this requires, omitting all strictly positive factors, … ►implying that, for $n\ge k$, the orthogonality of the $L_n^{(-k)}\left(x\right)$ with respect to the Laguerre weight function $x^{-k}{\mathrm{e}}^{-x}$, $x\in [0,\mathrm{\infty })$. …These results are proven in Everitt et al. (2004), via construction of a self-adjoint Sturm–Liouville operator which generates the $L_n^{(-k)}(x)$ polynomials, self-adjointness implying both orthogonality and completeness. … ►The resulting EOP’s, ${\widehat{L}}_n^{(k)}\left(x\right)$, $n=1,2,\mathrm{\dots }$ satisfy …

24: 23.2 Definitions and Periodic Properties

… ►The generators of a given lattice $𝕃$ are not unique. …where $a,b,c,d$ are integers, then $2{\chi }_1$, $2{\chi }_3$ are generators of $𝕃$ iff … ►When $z\notin 𝕃$ the functions are related by … ►When it is important to display the lattice with the functions they are denoted by $\mathrm{\wp }\left(z|𝕃\right)$, $\zeta \left(z|𝕃\right)$, and $\sigma \left(z|𝕃\right)$, respectively. … ►If $2{\omega }_1$, $2{\omega }_3$ is any pair of generators of $𝕃$, and ${\omega }_2$ is defined by (23.2.1), then …

25: Bibliography

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Exact linearization of a Painlevé transcendent. Phys. Rev. Lett. 38 (20), pp. 1103–1106.

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External Links:

Document, MathReview (Mark Adler)

Referenced by:

§32.11(ii), §32.13(i), §32.13(ii), §32.13(iii), §32.5.

Encodings:

BibTeX

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On the degrees of irreducible factors of higher order Bernoulli polynomials. Acta Arith. 62 (4), pp. 329–342.

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External Links:

ISSN 0065-1036, Pdf, MathReview (L. Skula), ZentralBlatt

Referenced by:

§24.12(iii).

Encodings:

BibTeX

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Repeated integrals and derivatives of $K$ Bessel functions. SIAM J. Math. Anal. 20 (1), pp. 169–175.

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External Links:

ISSN 0036-1410, Document, MathReview (A. Haimovici), ZentralBlatt

Referenced by:

§10.43(iii).

Encodings:

BibTeX

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Derivatives and integrals with respect to the order of the Struve functions ${𝐇}_{\nu }(x)$ and ${𝐋}_{\nu }(x)$ . J. Math. Anal. Appl. 137 (1), pp. 17–36.

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External Links:

ISSN 0022-247X, Document, MathReview (A. McD. Mercer), ZentralBlatt

Referenced by:

§11.4(vi), §11.7(iv).

Encodings:

BibTeX

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Note on the trivial zeros of Dirichlet $L$-functions. Proc. Amer. Math. Soc. 94 (1), pp. 29–30.

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External Links:

ISSN 0002-9939, FullText, MathReview (Jerzy Kaczorowski), ZentralBlatt

Referenced by:

(25.15.7), (25.15.8), §25.15(ii), §25.15.

Encodings:

BibTeX

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26: 18.41 Tables

… ►Abramowitz and Stegun (1964, Tables 22.4, 22.6, 22.11, and 22.13) tabulates $T_n\left(x\right)$, $U_n\left(x\right)$, $L_n\left(x\right)$, and $H_n\left(x\right)$ for $n=0(1)12$. The ranges of $x$ are $0.2(.2)1$ for $T_n\left(x\right)$ and $U_n\left(x\right)$, and $0.5,1,3,5,10$ for $L_n\left(x\right)$ and $H_n\left(x\right)$. … ►For $P_n\left(x\right)$, $L_n\left(x\right)$, and $H_n\left(x\right)$ see §3.5(v). …

27: 19.33 Triaxial Ellipsoids

… ►The external field and the induced magnetization together produce a uniform field inside the ellipsoid with strength $H/(1+L_c\chi )$, where $L_c$ is the demagnetizing factor, given in cgs units by ►

19.33.7 $$L_c=2\pi abc{\int }_0^{\mathrm{\infty }}\frac{d\lambda }{\sqrt{(a^2+\lambda )(b^2+\lambda ){(c^2+\lambda )}^3}}=V{R}_D(a^2,b^2,c^2).$$

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Symbols:

$R_D(x,y,z)$: elliptic integral symmetric in only two variables, $\pi$: the ratio of the circumference of a circle to its diameter, $dx$: differential of $x$ , $\int$: integral, $L_a$, $L_b$: factor and $V$: volume

Referenced by:

§19.15, §19.33(iii)

Permalink:

http://dlmf.nist.gov/19.33.E7

Encodings:

pMML, png, TeX

See also:

Annotations for §19.33(iii), §19.33 and Ch.19

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19.33.8 $$L_a+L_b+L_c=4\pi ,$$

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Symbols:

$\pi$: the ratio of the circumference of a circle to its diameter and $L_a$, $L_b$: factor

Permalink:

http://dlmf.nist.gov/19.33.E8

Encodings:

pMML, png, TeX

See also:

Annotations for §19.33(iii), §19.33 and Ch.19

►where $L_a$ and $L_b$ are obtained from $L_c$ by permutation of $a$, $b$, and $c$. …

28: 27.15 Chinese Remainder Theorem

… ►Their product $m$ has 20 digits, twice the number of digits in the data. …These numbers, in turn, are combined by the Chinese remainder theorem to obtain the final result $(modm)$, which is correct to 20 digits. …

29: William P. Reinhardt

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20 Theta Functions

… ►In November 2015, Reinhardt was named Senior Associate Editor of the DLMF and Associate Editor for Chapters 20, 22, and 23.

30: 11.15 Approximations

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Luke (1975, pp. 416–421) gives Chebyshev-series expansions for ${𝐇}_n\left(x\right)$, ${𝐋}_n\left(x\right)$, $0\le \left|x\right|\le 8$, and ${𝐇}_n\left(x\right)-Y_n\left(x\right)$, $x\ge 8$, for $n=0,1$; ${\int }_0^x{t}^{-m}{𝐇}_0\left(t\right)dt$, ${\int }_0^x{t}^{-m}{𝐋}_0\left(t\right)dt$, $0\le \left|x\right|\le 8$, $m=0,1$ and ${\int }_0^x({𝐇}_0\left(t\right)-Y_0\left(t\right))dt$, ${\int }_x^{\mathrm{\infty }}{t}^{-1}({𝐇}_0\left(t\right)-Y_0\left(t\right))dt$, $x\ge 8$; the coefficients are to 20D.

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MacLeod (1993) gives Chebyshev-series expansions for ${𝐋}_0\left(x\right)$, ${𝐋}_1\left(x\right)$, $0\le x\le 16$, and $I_0\left(x\right)-{𝐋}_0\left(x\right)$, $I_1\left(x\right)-{𝐋}_1\left(x\right)$, $x\ge 16$; the coefficients are to 20D.

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