Special mathematical functions.

The naming and numbering of the functions is taken from Matt Austern, (Draft) Technical Report on Standard Library Extensions, N1687=04-0127, September 10, 2004

Author: Created by Andras Zsenei on Mon Nov 8 2004

Special Functions from MathCore
double	ROOT::Math::erf (double x)
	Error function encountered in integrating the normal distribution.

double	ROOT::Math::erfc (double x)
	Complementary error function.

double	ROOT::Math::tgamma (double x)
	The gamma function is defined to be the extension of the factorial to real numbers.

double	ROOT::Math::lgamma (double x)
	Calculates the logarithm of the gamma function.

double	ROOT::Math::inc_gamma (double a, double x)
	Calculates the normalized (regularized) lower incomplete gamma function (lower integral)

double	ROOT::Math::inc_gamma_c (double a, double x)
	Calculates the normalized (regularized) upper incomplete gamma function (upper integral)

double	ROOT::Math::beta (double x, double y)
	Calculates the beta function.

double	ROOT::Math::inc_beta (double x, double a, double b)
	Calculates the normalized (regularized) incomplete beta function.

double	ROOT::Math::sinint (double x)
	Calculates the sine integral.

double	ROOT::Math::cosint (double x)
	Calculates the real part of the cosine integral Re(Ci).

Special Functions from MathMore
double	ROOT::Math::assoc_laguerre (unsigned n, double m, double x)
	Computes the generalized Laguerre polynomials for $ n \geq 0, m > -1 $.

double	ROOT::Math::assoc_legendre (unsigned l, unsigned m, double x)
	Computes the associated Legendre polynomials.

double	ROOT::Math::comp_ellint_1 (double k)
	Calculates the complete elliptic integral of the first kind.

double	ROOT::Math::comp_ellint_2 (double k)
	Calculates the complete elliptic integral of the second kind.

double	ROOT::Math::comp_ellint_3 (double n, double k)
	Calculates the complete elliptic integral of the third kind.

double	ROOT::Math::conf_hyperg (double a, double b, double z)
	Calculates the confluent hypergeometric functions of the first kind.

double	ROOT::Math::conf_hypergU (double a, double b, double z)
	Calculates the confluent hypergeometric functions of the second kind, known also as Kummer function of the second kind, it is related to the confluent hypergeometric functions of the first kind.

double	ROOT::Math::cyl_bessel_i (double nu, double x)
	Calculates the modified Bessel function of the first kind (also called regular modified (cylindrical) Bessel function).

double	ROOT::Math::cyl_bessel_j (double nu, double x)
	Calculates the (cylindrical) Bessel functions of the first kind (also called regular (cylindrical) Bessel functions).

double	ROOT::Math::cyl_bessel_k (double nu, double x)
	Calculates the modified Bessel functions of the second kind (also called irregular modified (cylindrical) Bessel functions).

double	ROOT::Math::cyl_neumann (double nu, double x)
	Calculates the (cylindrical) Bessel functions of the second kind (also called irregular (cylindrical) Bessel functions or (cylindrical) Neumann functions).

double	ROOT::Math::ellint_1 (double k, double phi)
	Calculates the incomplete elliptic integral of the first kind.

double	ROOT::Math::ellint_2 (double k, double phi)
	Calculates the complete elliptic integral of the second kind.

double	ROOT::Math::ellint_3 (double n, double k, double phi)
	Calculates the complete elliptic integral of the third kind.

double	ROOT::Math::expint (double x)
	Calculates the exponential integral.

double	ROOT::Math::hyperg (double a, double b, double c, double x)
	Calculates Gauss' hypergeometric function.

double	ROOT::Math::laguerre (unsigned n, double x)
	Calculates the Laguerre polynomials.

double	ROOT::Math::lambert_W0 (double x)
	Calculates the Lambert W function on branch 0.

double	ROOT::Math::lambert_Wm1 (double x)
	Calculates the Lambert W function on branch -1.

double	ROOT::Math::legendre (unsigned l, double x)
	Calculates the Legendre polynomials.

double	ROOT::Math::riemann_zeta (double x)
	Calculates the Riemann zeta function.

double	ROOT::Math::sph_bessel (unsigned n, double x)
	Calculates the spherical Bessel functions of the first kind (also called regular spherical Bessel functions).

double	ROOT::Math::sph_legendre (unsigned l, unsigned m, double theta)
	Computes the spherical (normalized) associated Legendre polynomials, or spherical harmonic without azimuthal dependence ( $e^(im\phi)$).

double	ROOT::Math::sph_neumann (unsigned n, double x)
	Calculates the spherical Bessel functions of the second kind (also called irregular spherical Bessel functions or spherical Neumann functions).

double	ROOT::Math::airy_Ai (double x)
	Calculates the Airy function Ai.

double	ROOT::Math::airy_Bi (double x)
	Calculates the Airy function Bi.

double	ROOT::Math::airy_Ai_deriv (double x)
	Calculates the derivative of the Airy function Ai.

double	ROOT::Math::airy_Bi_deriv (double x)
	Calculates the derivative of the Airy function Bi.

double	ROOT::Math::airy_zero_Ai (unsigned int s)
	Calculates the zeroes of the Airy function Ai.

double	ROOT::Math::airy_zero_Bi (unsigned int s)
	Calculates the zeroes of the Airy function Bi.

double	ROOT::Math::airy_zero_Ai_deriv (unsigned int s)
	Calculates the zeroes of the derivative of the Airy function Ai.

double	ROOT::Math::airy_zero_Bi_deriv (unsigned int s)
	Calculates the zeroes of the derivative of the Airy function Bi.

double	ROOT::Math::wigner_3j (int two_ja, int two_jb, int two_jc, int two_ma, int two_mb, int two_mc)
	Calculates the Wigner 3j coupling coefficients.

double	ROOT::Math::wigner_6j (int two_ja, int two_jb, int two_jc, int two_jd, int two_je, int two_jf)
	Calculates the Wigner 6j coupling coefficients.

double	ROOT::Math::wigner_9j (int two_ja, int two_jb, int two_jc, int two_jd, int two_je, int two_jf, int two_jg, int two_jh, int two_ji)
	Calculates the Wigner 9j coupling coefficients.

double	ROOT::Math::expint_n (int n, double x)

Function Documentation

◆ airy_Ai()

double ROOT::Math::airy_Ai ( double x )

Calculates the Airy function Ai.

\[ Ai(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} \cos(xt + t^3/3) dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 401 of file SpecFuncMathMore.cxx.

◆ airy_Ai_deriv()

double ROOT::Math::airy_Ai_deriv ( double x )

Calculates the derivative of the Airy function Ai.

\[ Ai(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} \cos(xt + t^3/3) dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 417 of file SpecFuncMathMore.cxx.

◆ airy_Bi()

double ROOT::Math::airy_Bi ( double x )

Calculates the Airy function Bi.

\[ Bi(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} [\exp(xt-t^3/3) + \cos(xt + t^3/3)] dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 409 of file SpecFuncMathMore.cxx.

◆ airy_Bi_deriv()

double ROOT::Math::airy_Bi_deriv ( double x )

Calculates the derivative of the Airy function Bi.

\[ Bi(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} [\exp(xt-t^3/3) + \cos(xt + t^3/3)] dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 425 of file SpecFuncMathMore.cxx.

◆ airy_zero_Ai()

double ROOT::Math::airy_zero_Ai ( unsigned int s )

Calculates the zeroes of the Airy function Ai.

\[ Ai(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} \cos(xt + t^3/3) dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 433 of file SpecFuncMathMore.cxx.

◆ airy_zero_Ai_deriv()

double ROOT::Math::airy_zero_Ai_deriv ( unsigned int s )

Calculates the zeroes of the derivative of the Airy function Ai.

\[ Ai(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} \cos(xt + t^3/3) dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 449 of file SpecFuncMathMore.cxx.

◆ airy_zero_Bi()

double ROOT::Math::airy_zero_Bi ( unsigned int s )

Calculates the zeroes of the Airy function Bi.

\[ Bi(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} [\exp(xt-t^3/3) + \cos(xt + t^3/3)] dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 441 of file SpecFuncMathMore.cxx.

◆ airy_zero_Bi_deriv()

double ROOT::Math::airy_zero_Bi_deriv ( unsigned int s )

Calculates the zeroes of the derivative of the Airy function Bi.

\[ Bi(x) = \frac{1}{\pi} \int\limits_{0}^{\infty} [\exp(xt-t^3/3) + \cos(xt + t^3/3)] dt \]

For detailed description see Mathworld and Abramowitz&Stegun, Sect. 10.4. The implementation used is that of GSL.

Definition at line 457 of file SpecFuncMathMore.cxx.

◆ assoc_laguerre()

double ROOT::Math::assoc_laguerre	(	unsigned	n,
		double	m,
		double	x
	)

Computes the generalized Laguerre polynomials for $ n \geq 0, m > -1 $.

They are defined in terms of the confluent hypergeometric function. For integer values of m they can be defined in terms of the Laguerre polynomials $L_n(x)$:

\[ L_{n}^{m}(x) = (-1)^{m} \frac{d^m}{dx^m} L_{n+m}(x) \]

For detailed description see Mathworld. The implementation used is that of GSL.

This function is an extension of C++0x, also consistent in GSL, Abramowitz and Stegun 1972 and MatheMathica that uses non-integer values for m. C++0x calls for 'int m', more restrictive than necessary. The definition for was incorrect in 'n1687.pdf', but fixed in n1836.pdf, the most recent draft as of 2007-07-01

Definition at line 42 of file SpecFuncMathMore.cxx.

◆ assoc_legendre()

double ROOT::Math::assoc_legendre	(	unsigned	l,
		unsigned	m,
		double	x
	)

Computes the associated Legendre polynomials.

\[ P_{l}^{m}(x) = (1-x^2)^{m/2} \frac{d^m}{dx^m} P_{l}(x) \]

with $m \geq 0$, $ l \geq m $ and $ |x|<1 $. There are two sign conventions for associated Legendre polynomials. As is the case with the above formula, some authors (e.g., Arfken 1985, pp. 668-669) omit the Condon-Shortley phase $(-1)^m$, while others include it (e.g., Abramowitz and Stegun 1972). One possible way to distinguish the two conventions is due to Abramowitz and Stegun (1972, p. 332), who use the notation

\[ P_{lm} (x) = (-1)^m P_{l}^{m} (x)\]

to distinguish the two. For detailed description see Mathworld. The implementation used is that of GSL.

The definition uses is the one of C++0x, $ P_{lm}$, while GSL and MatheMatica use the $P_{l}^{m}$ definition. Note that C++0x and GSL definitions agree instead for the normalized associated Legendre polynomial, sph_legendre(l,m,theta).

Definition at line 53 of file SpecFuncMathMore.cxx.

◆ beta()

double ROOT::Math::beta	(	double	x,
		double	y
	)

Calculates the beta function.

\[ B(x,y) = \frac{\Gamma(x) \Gamma(y)}{\Gamma(x+y)} \]

for x>0 and y>0. For detailed description see Mathworld.

Definition at line 111 of file SpecFuncMathCore.cxx.

◆ comp_ellint_1()

double ROOT::Math::comp_ellint_1 ( double k )

Calculates the complete elliptic integral of the first kind.

\[ K(k) = F(k, \pi / 2) = \int_{0}^{\pi /2} \frac{d \theta}{\sqrt{1 - k^2 \sin^2{\theta}}} \]

with $0 \leq k^2 \leq 1$. For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 70 of file SpecFuncMathMore.cxx.

◆ comp_ellint_2()

double ROOT::Math::comp_ellint_2 ( double k )

Calculates the complete elliptic integral of the second kind.

\[ E(k) = E(k , \pi / 2) = \int_{0}^{\pi /2} \sqrt{1 - k^2 \sin^2{\theta}} d \theta \]

with $0 \leq k^2 \leq 1$. For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 81 of file SpecFuncMathMore.cxx.

◆ comp_ellint_3()

double ROOT::Math::comp_ellint_3	(	double	n,
		double	k
	)

Calculates the complete elliptic integral of the third kind.

Complete elliptic integral of the third kind.

\[ \Pi (n, k, \pi / 2) = \int_{0}^{\pi /2} \frac{d \theta}{(1 - n \sin^2{\theta})\sqrt{1 - k^2 \sin^2{\theta}}} \]

with $0 \leq k^2 \leq 1$. There are two sign conventions for elliptic integrals of the third kind. Some authors (Abramowitz and Stegun, Mathworld, C++ standard proposal) use the above formula, while others (GSL, Planetmath and CERNLIB) use the + sign in front of n in the denominator. In order to be C++ compliant, the present library uses the former convention. The implementation used is that of GSL.

There are two different definitions used for the elliptic integral of the third kind:

\[ P(\phi,k,n) = \int_0^\phi \frac{dt}{(1 + n \sin^2{t})\sqrt{1 - k^2 \sin^2{t}}} \]

and

\[ P(\phi,k,n) = \int_0^\phi \frac{dt}{(1 - n \sin^2{t})\sqrt{1 - k^2 \sin^2{t}}} \]

the former is adopted by

GSL http://www.gnu.org/software/gsl/manual/gsl-ref_7.html#SEC95
Planetmath http://planetmath.org/encyclopedia/EllipticIntegralsAndJacobiEllipticFunctions.html
CERNLIB https://cern-tex.web.cern.ch/cern-tex/shortwrupsdir/c346/top.html

while the latter is used by
Abramowitz and Stegun
Mathematica http://mathworld.wolfram.com/EllipticIntegraloftheThirdKind.html
C++ standard http://www.open-std.org/jtc1/sc22/wg21/docs/papers/2004/n1687.pdf

in order to be C++ compliant, we decided to use the latter, hence the change of the sign in the function call to GSL.

Definition at line 133 of file SpecFuncMathMore.cxx.

◆ conf_hyperg()

double ROOT::Math::conf_hyperg	(	double	a,
		double	b,
		double	z
	)

Calculates the confluent hypergeometric functions of the first kind.

\[ _{1}F_{1}(a;b;z) = \frac{\Gamma(b)}{\Gamma(a)} \sum_{n=0}^{\infty} \frac{\Gamma(a+n)}{\Gamma(b+n)} \frac{z^n}{n!} \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 144 of file SpecFuncMathMore.cxx.

◆ conf_hypergU()

double ROOT::Math::conf_hypergU	(	double	a,
		double	b,
		double	z
	)

Calculates the confluent hypergeometric functions of the second kind, known also as Kummer function of the second kind, it is related to the confluent hypergeometric functions of the first kind.

\[ U(a,b,z) = \frac{ \pi}{ \sin{\pi b } } \left[ \frac{ _{1}F_{1}(a,b,z) } {\Gamma(a-b+1) } - \frac{ z^{1-b} { _{1}F_{1}}(a-b+1,2-b,z)}{\Gamma(a)} \right] \]

For detailed description see Mathworld. The implementation used is that of GSL. This function is not part of the C++ standard proposal

Definition at line 152 of file SpecFuncMathMore.cxx.

◆ cosint()

double ROOT::Math::cosint ( double x )

Calculates the real part of the cosine integral Re(Ci).

For x<0, the imaginary part is \pi i and has to be added by the user, for x>0 the imaginary part of Ci(x) is 0.

\[ Ci(x) = - \int_{x}^{\infty} \frac{\cos t}{t} dt = \gamma + \ln x + \int_{0}^{x} \frac{\cos t - 1}{t} dt\]

For detailed description see Mathworld. The implementation used is that of CERNLIB, based on Y.L. Luke, The special functions and their approximations, v.II, (Academic Press, New York l969) 325-326.

Definition at line 212 of file SpecFuncMathCore.cxx.

◆ cyl_bessel_i()

double ROOT::Math::cyl_bessel_i	(	double	nu,
		double	x
	)

Calculates the modified Bessel function of the first kind (also called regular modified (cylindrical) Bessel function).

\[ I_{\nu} (x) = i^{-\nu} J_{\nu}(ix) = \sum_{k=0}^{\infty} \frac{(\frac{1}{2}x)^{\nu + 2k}}{k! \Gamma(\nu + k + 1)} \]

for $x>0, \nu > 0$. For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 163 of file SpecFuncMathMore.cxx.

◆ cyl_bessel_j()

double ROOT::Math::cyl_bessel_j	(	double	nu,
		double	x
	)

Calculates the (cylindrical) Bessel functions of the first kind (also called regular (cylindrical) Bessel functions).

\[ J_{\nu} (x) = \sum_{k=0}^{\infty} \frac{(-1)^k(\frac{1}{2}x)^{\nu + 2k}}{k! \Gamma(\nu + k + 1)} \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 174 of file SpecFuncMathMore.cxx.

◆ cyl_bessel_k()

double ROOT::Math::cyl_bessel_k	(	double	nu,
		double	x
	)

Calculates the modified Bessel functions of the second kind (also called irregular modified (cylindrical) Bessel functions).

\[ K_{\nu} (x) = \frac{\pi}{2} i^{\nu + 1} (J_{\nu} (ix) + iN(ix)) = \left\{ \begin{array}{cl} \frac{\pi}{2} \frac{I_{-\nu}(x) - I_{\nu}(x)}{\sin{\nu \pi}} & \mbox{for non-integral $\nu$} \\ \frac{\pi}{2} \lim{\mu \to \nu} \frac{I_{-\mu}(x) - I_{\mu}(x)}{\sin{\mu \pi}} & \mbox{for integral $\nu$} \end{array} \right. \]

for $x>0, \nu > 0$. For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 185 of file SpecFuncMathMore.cxx.

◆ cyl_neumann()

double ROOT::Math::cyl_neumann	(	double	nu,
		double	x
	)

Calculates the (cylindrical) Bessel functions of the second kind (also called irregular (cylindrical) Bessel functions or (cylindrical) Neumann functions).

\[ N_{\nu} (x) = Y_{\nu} (x) = \left\{ \begin{array}{cl} \frac{J_{\nu} \cos{\nu \pi}-J_{-\nu}(x)}{\sin{\nu \pi}} & \mbox{for non-integral $\nu$} \\ \lim{\mu \to \nu} \frac{J_{\mu} \cos{\mu \pi}-J_{-\mu}(x)}{\sin{\mu \pi}} & \mbox{for integral $\nu$} \end{array} \right. \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 197 of file SpecFuncMathMore.cxx.

◆ ellint_1()

double ROOT::Math::ellint_1	(	double	k,
		double	phi
	)

Calculates the incomplete elliptic integral of the first kind.

\[ F(k, \phi) = \int_{0}^{\phi} \frac{d \theta}{\sqrt{1 - k^2 \sin^2{\theta}}} \]

with $0 \leq k^2 \leq 1$. For detailed description see Mathworld. The implementation used is that of GSL.

Parameters

k
phi	angle in radians

Definition at line 209 of file SpecFuncMathMore.cxx.

◆ ellint_2()

double ROOT::Math::ellint_2	(	double	k,
		double	phi
	)

Calculates the complete elliptic integral of the second kind.

\[ E(k , \phi) = \int_{0}^{\phi} \sqrt{1 - k^2 \sin^2{\theta}} d \theta \]

with $0 \leq k^2 \leq 1$. For detailed description see Mathworld. The implementation used is that of GSL.

Parameters

k
phi	angle in radians

Definition at line 221 of file SpecFuncMathMore.cxx.

◆ ellint_3()

double ROOT::Math::ellint_3	(	double	n,
		double	k,
		double	phi
	)

Calculates the complete elliptic integral of the third kind.

Incomplete elliptic integral of the third kind.

\[ \Pi (n, k, \phi) = \int_{0}^{\phi} \frac{d \theta}{(1 - n \sin^2{\theta})\sqrt{1 - k^2 \sin^2{\theta}}} \]

with $0 \leq k^2 \leq 1$. There are two sign conventions for elliptic integrals of the third kind. Some authors (Abramowitz and Stegun, Mathworld, C++ standard proposal) use the above formula, while others (GSL, Planetmath and CERNLIB) use the + sign in front of n in the denominator. In order to be C++ compliant, the present library uses the former convention. The implementation used is that of GSL.

Parameters

n
k
phi	angle in radians

There are two different definitions used for the elliptic integral of the third kind:

\[ P(\phi,k,n) = \int_0^\phi \frac{dt}{(1 + n \sin^2{t})\sqrt{1 - k^2 \sin^2{t}}} \]

and

\[ P(\phi,k,n) = \int_0^\phi \frac{dt}{(1 - n \sin^2{t})\sqrt{1 - k^2 \sin^2{t}}} \]

the former is adopted by

GSL http://www.gnu.org/software/gsl/manual/gsl-ref_7.html#SEC95
Planetmath http://planetmath.org/encyclopedia/EllipticIntegralsAndJacobiEllipticFunctions.html
CERNLIB https://cern-tex.web.cern.ch/cern-tex/shortwrupsdir/c346/top.html

while the latter is used by
Abramowitz and Stegun
Mathematica http://mathworld.wolfram.com/EllipticIntegraloftheThirdKind.html
C++ standard http://www.open-std.org/jtc1/sc22/wg21/docs/papers/2004/n1687.pdf

in order to be C++ compliant, we decided to use the latter, hence the change of the sign in the function call to GSL.

Definition at line 275 of file SpecFuncMathMore.cxx.

◆ erf()

double ROOT::Math::erf ( double x )

Error function encountered in integrating the normal distribution.

\[ erf(x) = \frac{2}{\sqrt{\pi}} \int_{0}^{x} e^{-t^2} dt \]

For detailed description see Mathworld. The implementation used is that of GSL. This function is provided only for convenience, in case your standard C++ implementation does not support it. If it does, please use these standard version!

Definition at line 59 of file SpecFuncMathCore.cxx.

◆ erfc()

double ROOT::Math::erfc ( double x )

Complementary error function.

\[ erfc(x) = 1 - erf(x) = \frac{2}{\sqrt{\pi}} \int_{x}^{\infty} e^{-t^2} dt \]

For detailed description see Mathworld. The implementation used is that of Cephes from S. Moshier.

Definition at line 44 of file SpecFuncMathCore.cxx.

◆ expint()

double ROOT::Math::expint ( double x )

Calculates the exponential integral.

\[ Ei(x) = - \int_{-x}^{\infty} \frac{e^{-t}}{t} dt \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 286 of file SpecFuncMathMore.cxx.

◆ expint_n()

double ROOT::Math::expint_n	(	int	n,
		double	x
	)

Definition at line 295 of file SpecFuncMathMore.cxx.

◆ hyperg()

double ROOT::Math::hyperg	(	double	a,
		double	b,
		double	c,
		double	x
	)

Calculates Gauss' hypergeometric function.

\[ _{2}F_{1}(a,b;c;x) = \frac{\Gamma(c)}{\Gamma(a) \Gamma(b)} \sum_{n=0}^{\infty} \frac{\Gamma(a+n)\Gamma(b+n)}{\Gamma(c+n)} \frac{x^n}{n!} \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 315 of file SpecFuncMathMore.cxx.

◆ inc_beta()

double ROOT::Math::inc_beta	(	double	x,
		double	a,
		double	b
	)

Calculates the normalized (regularized) incomplete beta function.

\[ B(x, a, b ) = \frac{ \int_{0}^{x} u^{a-1} (1-u)^{b-1} du } { B(a,b) } \]

for 0<=x<=1, a>0, and b>0. For detailed description see Mathworld. The implementation used is that of Cephes from S. Moshier.

Definition at line 115 of file SpecFuncMathCore.cxx.

◆ inc_gamma()

double ROOT::Math::inc_gamma	(	double	a,
		double	x
	)

Calculates the normalized (regularized) lower incomplete gamma function (lower integral)

\[ P(a, x) = \frac{ 1} {\Gamma(a) } \int_{0}^{x} t^{a-1} e^{-t} dt \]

For a detailed description see Mathworld. The implementation used is that of Cephes from S. Moshier. In this implementation both a and x must be positive. If a is negative 1.0 is returned for every x. This is correct only if a is negative integer. For a>0 and x<0 0 is returned (this is correct only for a>0 and x=0).

Definition at line 99 of file SpecFuncMathCore.cxx.

◆ inc_gamma_c()

double ROOT::Math::inc_gamma_c	(	double	a,
		double	x
	)

Calculates the normalized (regularized) upper incomplete gamma function (upper integral)

\[ Q(a, x) = \frac{ 1} {\Gamma(a) } \int_{x}^{\infty} t^{a-1} e^{-t} dt \]

For a detailed description see Mathworld. The implementation used is that of Cephes from S. Moshier. In this implementation both a and x must be positive. If a is negative, 0 is returned for every x. This is correct only if a is negative integer. For a>0 and x<0 1 is returned (this is correct only for a>0 and x=0).

Definition at line 103 of file SpecFuncMathCore.cxx.

◆ laguerre()

double ROOT::Math::laguerre	(	unsigned	n,
		double	x
	)

Calculates the Laguerre polynomials.

\[ P_{l}(x) = \frac{ e^x}{n!} \frac{d^n}{dx^n} (x^n - e^{-x}) \]

for $x \geq 0 $ in the Rodrigues representation. They corresponds to the associated Laguerre polynomial of order m=0. See Abramowitz and Stegun, (22.5.16) For detailed description see Mathworld. The are implemented using the associated Laguerre polynomial of order m=0.

Definition at line 326 of file SpecFuncMathMore.cxx.

◆ lambert_W0()

double ROOT::Math::lambert_W0 ( double x )

Calculates the Lambert W function on branch 0.

The Lambert W functions are defined to be the solution of the equation

\[ W(x) \exp(W(x)) = x \]

For detailed description see Mathworld or Wikipedia.

This function implements the Lambert W function on branch 0, which is real valued and defined for $ x \geq -1/e $ with $ W_0(x) \geq -1 $.

Definition at line 333 of file SpecFuncMathMore.cxx.

◆ lambert_Wm1()

double ROOT::Math::lambert_Wm1 ( double x )

Calculates the Lambert W function on branch -1.

The Lambert W functions are defined to be the solution of the equation

\[ W(x) \exp(W(x)) = x \]

For detailed description see Mathworld or Wikipedia.

This function implements the Lambert W function on branch -1, which is real valued and defined for $ -1/e \seq x < 0 $ with $ W_{-1}(x) \seq -1 $.

Definition at line 340 of file SpecFuncMathMore.cxx.

◆ legendre()

double ROOT::Math::legendre	(	unsigned	l,
		double	x
	)

Calculates the Legendre polynomials.

\[ P_{l}(x) = \frac{1}{2^l l!} \frac{d^l}{dx^l} (x^2 - 1)^l \]

for $l \geq 0, |x|\leq1$ in the Rodrigues representation. For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 348 of file SpecFuncMathMore.cxx.

◆ lgamma()

double ROOT::Math::lgamma ( double x )

Calculates the logarithm of the gamma function.

The implementation used is that of Cephes from S. Moshier.

Definition at line 74 of file SpecFuncMathCore.cxx.

◆ riemann_zeta()

double ROOT::Math::riemann_zeta ( double x )

Calculates the Riemann zeta function.

\[ \zeta (x) = \left\{ \begin{array}{cl} \sum_{k=1}^{\infty}k^{-x} & \mbox{for $x > 1$} \\ 2^x \pi^{x-1} \sin{(\frac{1}{2}\pi x)} \Gamma(1-x) \zeta (1-x) & \mbox{for $x < 1$} \end{array} \right. \]

For detailed description see Mathworld. The implementation used is that of GSL.

CHECK WHETHER THE IMPLEMENTATION CALCULATES X<1

Definition at line 359 of file SpecFuncMathMore.cxx.

◆ sinint()

double ROOT::Math::sinint ( double x )

Calculates the sine integral.

\[ Si(x) = - \int_{0}^{x} \frac{\sin t}{t} dt \]

For detailed description see Mathworld. The implementation used is that of CERNLIB, based on Y.L. Luke, The special functions and their approximations, v.II, (Academic Press, New York l969) 325-326.

Definition at line 122 of file SpecFuncMathCore.cxx.

◆ sph_bessel()

double ROOT::Math::sph_bessel	(	unsigned	n,
		double	x
	)

Calculates the spherical Bessel functions of the first kind (also called regular spherical Bessel functions).

\[ j_{n}(x) = \sqrt{\frac{\pi}{2x}} J_{n+1/2}(x) \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 370 of file SpecFuncMathMore.cxx.

◆ sph_legendre()

double ROOT::Math::sph_legendre	(	unsigned	l,
		unsigned	m,
		double	theta
	)

Computes the spherical (normalized) associated Legendre polynomials, or spherical harmonic without azimuthal dependence ( $e^(im\phi)$).

\[ Y_l^m(theta,0) = \sqrt{(2l+1)/(4\pi)} \sqrt{(l-m)!/(l+m)!} P_l^m(cos \theta) \]

for $m \geq 0, l \geq m$, where the Condon-Shortley phase $(-1)^m$ is included in P_l^m(x) This function is consistent with both C++0x and GSL, even though there is a discrepancy in where to include the phase. There is no reference in Abramowitz and Stegun.

Definition at line 381 of file SpecFuncMathMore.cxx.

◆ sph_neumann()

double ROOT::Math::sph_neumann	(	unsigned	n,
		double	x
	)

Calculates the spherical Bessel functions of the second kind (also called irregular spherical Bessel functions or spherical Neumann functions).

\[ n_n(x) = y_n(x) = \sqrt{\frac{\pi}{2x}} N_{n+1/2}(x) \]

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 393 of file SpecFuncMathMore.cxx.

◆ tgamma()

double ROOT::Math::tgamma ( double x )

The gamma function is defined to be the extension of the factorial to real numbers.

\[ \Gamma(x) = \int_{0}^{\infty} t^{x-1} e^{-t} dt \]

For detailed description see Mathworld. The implementation used is that of Cephes from S. Moshier.

Definition at line 89 of file SpecFuncMathCore.cxx.

◆ wigner_3j()

double ROOT::Math::wigner_3j	(	int	two_ja,
		int	two_jb,
		int	two_jc,
		int	two_ma,
		int	two_mb,
		int	two_mc
	)

Calculates the Wigner 3j coupling coefficients.

    (ja jb jc
    ma mb mc)

where ja,ma,...etc are integers or half integers. The function takes as input arguments only integers which corresponds to half integer units, e.g two_ja = 2 * ja

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 465 of file SpecFuncMathMore.cxx.

◆ wigner_6j()

double ROOT::Math::wigner_6j	(	int	two_ja,
		int	two_jb,
		int	two_jc,
		int	two_jd,
		int	two_je,
		int	two_jf
	)

Calculates the Wigner 6j coupling coefficients.

    (ja jb jc
     jd je jf)

where ja,jb,...etc are integers or half integers. The function takes as input arguments only integers which corresponds to half integer units, e.g two_ja = 2 * ja

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 469 of file SpecFuncMathMore.cxx.

◆ wigner_9j()

double ROOT::Math::wigner_9j	(	int	two_ja,
		int	two_jb,
		int	two_jc,
		int	two_jd,
		int	two_je,
		int	two_jf,
		int	two_jg,
		int	two_jh,
		int	two_ji
	)

Calculates the Wigner 9j coupling coefficients.

    (ja jb jc
     jd je jf
     jg jh ji)

where ja,jb...etc are integers or half integers. The function takes as input arguments only integers which corresponds to half integer units, e.g two_ja = 2 * ja

For detailed description see Mathworld. The implementation used is that of GSL.

Definition at line 473 of file SpecFuncMathMore.cxx.

Special Functions from MathCore

Special Functions from MathMore

Function Documentation

◆ airy_Ai()

◆ airy_Ai_deriv()

◆ airy_Bi()

◆ airy_Bi_deriv()

◆ airy_zero_Ai()

◆ airy_zero_Ai_deriv()

◆ airy_zero_Bi()

◆ airy_zero_Bi_deriv()

◆ assoc_laguerre()

◆ assoc_legendre()

◆ beta()

◆ comp_ellint_1()

◆ comp_ellint_2()

◆ comp_ellint_3()

◆ conf_hyperg()

◆ conf_hypergU()

◆ cosint()

◆ cyl_bessel_i()

◆ cyl_bessel_j()

◆ cyl_bessel_k()

◆ cyl_neumann()

◆ ellint_1()

◆ ellint_2()

◆ ellint_3()

◆ erf()

◆ erfc()

◆ expint()

◆ expint_n()

◆ hyperg()

◆ inc_beta()

◆ inc_gamma()

◆ inc_gamma_c()

◆ laguerre()

◆ lambert_W0()

◆ lambert_Wm1()

◆ legendre()

◆ lgamma()

◆ riemann_zeta()

◆ sinint()

◆ sph_bessel()

◆ sph_legendre()

◆ sph_neumann()

◆ tgamma()

◆ wigner_3j()

◆ wigner_6j()

◆ wigner_9j()