Difference between revisions of "Gamma-correlation"
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+ | The two-dimensional distribution of non-negative random dependent variables $ X _ {1} $ | ||
+ | and $ X _ {2} $ | ||
+ | defined by the density | ||
+ | |||
+ | $$ | ||
+ | p ( x _ {1} , x _ {2} ) = \ | ||
+ | p _ {1} ( x _ {1} ) p _ {2} ( x _ {2} ) | ||
+ | \sum _ {k = 0 } ^ \infty | ||
+ | c _ {k} a _ {k} L _ {k} ^ {\alpha _ {1} } | ||
+ | ( x _ {1} ) L _ {k} ^ {\alpha _ {2} } ( x _ {2} ), | ||
+ | $$ | ||
where | where | ||
− | < | + | $$ |
+ | 0 \leq x _ \nu < \infty ; \ \ | ||
+ | \alpha _ \nu \geq \gamma > - 1; \ \ | ||
+ | \rho _ \nu ( x _ \nu ) = \ | ||
+ | x _ \nu ^ {\alpha _ \nu } | ||
+ | |||
+ | \frac{e ^ {- x _ \nu } }{\Gamma ( \alpha _ \nu + 1) } | ||
+ | , | ||
+ | $$ | ||
+ | |||
+ | $ L _ {k} ^ {\alpha _ \nu } ( x _ \nu ) $ | ||
+ | are the [[Laguerre polynomials|Laguerre polynomials]], orthonormalized on the positive semi-axis with weight $ p _ \nu ( x _ \nu ) $, | ||
+ | $ \nu = 1, 2 $; | ||
− | + | $$ | |
+ | a _ {k} = \ | ||
− | + | \frac{\Gamma ( \gamma + k + 1) }{\Gamma ( \gamma + 1) } | |
− | + | \sqrt { | |
+ | \frac{\Gamma ( \alpha _ {1} + 1) \Gamma ( \alpha _ {2} + 1) }{\Gamma ( \alpha _ {1} + k + 1) \Gamma ( \alpha _ {2} + k + 1) } | ||
+ | } ; | ||
+ | $$ | ||
− | + | $$ | |
+ | c _ {k} = \int\limits _ { 0 } ^ { 1 } \lambda ^ {k} dF ( \lambda ),\ k = 0, 1 ,\dots; | ||
+ | $$ | ||
− | + | and $ F ( \lambda ) $ | |
+ | is an arbitrary distribution function on the segment $ [ 0, 1] $. | ||
+ | The correlation coefficient between $ X _ {1} $ | ||
+ | and $ X _ {2} $ | ||
+ | is $ c _ {1} { {( \gamma + 1) } / \sqrt {( \alpha _ {1} + 1 )( \alpha _ {2} + 1 ) } } $. | ||
+ | If $ \alpha _ {1} = \alpha _ {2} = \gamma $, | ||
+ | a symmetric gamma-correlation is obtained; in such a case $ a _ {k} = 1 $, | ||
+ | $ k = 0, 1 \dots $ | ||
+ | and the form of the corresponding characteristic function is | ||
− | + | $$ | |
+ | \phi ( t _ {1} , t _ {2} ) = \ | ||
+ | \int\limits _ { 0 } ^ { 1 } | ||
− | + | \frac{dF ( \lambda ) }{[ 1 - it _ {1} - it _ {2} - t _ {1} t _ {2} ( 1 - \lambda )] ^ {1 + \gamma } } | |
+ | . | ||
+ | $$ | ||
− | + | If $ F ( \lambda ) $ | |
+ | is such that $ {\mathsf P} \{ \lambda = R \} = 1 $, | ||
+ | then $ c _ {k} = R ^ {k} $, | ||
+ | $ \phi ( t _ {1} , t _ {2} ) = [ 1 - it _ {1} - it _ {2} - t _ {1} t _ {2} ( 1 - R)] ^ {- 1- \gamma } $, | ||
+ | and $ R $ | ||
+ | is the [[Correlation coefficient|correlation coefficient]] between $ X _ {1} $ | ||
+ | and $ X _ {2} $( | ||
+ | $ 0 \leq R \leq 1 $). | ||
+ | In this last case the density series can be summed using the formula (cf. [[#References|[2]]]): | ||
− | + | $$ | |
+ | p ( x _ {1} , x _ {2} ) = \ | ||
+ | |||
+ | \frac{( x _ {1} x _ {2} ) ^ \gamma e ^ {- x _ {1} - x _ {2} } }{\Gamma ^ {2} ( \gamma + 1) } | ||
+ | |||
+ | \sum _ {k = 0 } ^ \infty | ||
+ | R ^ {k} L _ {k} ^ \gamma ( x _ {1} ) L _ {k} ^ \gamma ( x _ {2} ) = | ||
+ | $$ | ||
+ | |||
+ | $$ | ||
+ | = \ | ||
+ | |||
+ | \frac{e ^ {- ( x _ {1} + x _ {2} ) / ( 1 - R) } }{( 1 - R) \Gamma | ||
+ | ( \gamma + 1) } | ||
+ | \left ( | ||
+ | \frac{x _ {1} x _ {2} }{R } | ||
+ | \right ) ^ {\gamma / 2 } I _ \gamma \left ( | ||
+ | \frac{2 \sqrt | ||
+ | {x _ {1} x _ {2} R } }{1 - R } | ||
+ | \right ) , | ||
+ | $$ | ||
+ | |||
+ | where $ I _ \gamma $ | ||
+ | is the Bessel function of an imaginary argument [[#References|[2]]]. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> I.O. Sarmanov, ''Trudy Gidrologichesk. Inst.'' , '''162''' (1969) pp. 37–61</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> W. Myller-Lebedeff, "Die Theorie der Integralgleichungen in Anwendung auf einige Reihenentwicklungen" ''Math. Ann.'' , '''64''' (1907) pp. 388–416</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> I.O. Sarmanov, ''Trudy Gidrologichesk. Inst.'' , '''162''' (1969) pp. 37–61</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> W. Myller-Lebedeff, "Die Theorie der Integralgleichungen in Anwendung auf einige Reihenentwicklungen" ''Math. Ann.'' , '''64''' (1907) pp. 388–416</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== |
Latest revision as of 19:41, 5 June 2020
The two-dimensional distribution of non-negative random dependent variables $ X _ {1} $
and $ X _ {2} $
defined by the density
$$ p ( x _ {1} , x _ {2} ) = \ p _ {1} ( x _ {1} ) p _ {2} ( x _ {2} ) \sum _ {k = 0 } ^ \infty c _ {k} a _ {k} L _ {k} ^ {\alpha _ {1} } ( x _ {1} ) L _ {k} ^ {\alpha _ {2} } ( x _ {2} ), $$
where
$$ 0 \leq x _ \nu < \infty ; \ \ \alpha _ \nu \geq \gamma > - 1; \ \ \rho _ \nu ( x _ \nu ) = \ x _ \nu ^ {\alpha _ \nu } \frac{e ^ {- x _ \nu } }{\Gamma ( \alpha _ \nu + 1) } , $$
$ L _ {k} ^ {\alpha _ \nu } ( x _ \nu ) $ are the Laguerre polynomials, orthonormalized on the positive semi-axis with weight $ p _ \nu ( x _ \nu ) $, $ \nu = 1, 2 $;
$$ a _ {k} = \ \frac{\Gamma ( \gamma + k + 1) }{\Gamma ( \gamma + 1) } \sqrt { \frac{\Gamma ( \alpha _ {1} + 1) \Gamma ( \alpha _ {2} + 1) }{\Gamma ( \alpha _ {1} + k + 1) \Gamma ( \alpha _ {2} + k + 1) } } ; $$
$$ c _ {k} = \int\limits _ { 0 } ^ { 1 } \lambda ^ {k} dF ( \lambda ),\ k = 0, 1 ,\dots; $$
and $ F ( \lambda ) $ is an arbitrary distribution function on the segment $ [ 0, 1] $. The correlation coefficient between $ X _ {1} $ and $ X _ {2} $ is $ c _ {1} { {( \gamma + 1) } / \sqrt {( \alpha _ {1} + 1 )( \alpha _ {2} + 1 ) } } $. If $ \alpha _ {1} = \alpha _ {2} = \gamma $, a symmetric gamma-correlation is obtained; in such a case $ a _ {k} = 1 $, $ k = 0, 1 \dots $ and the form of the corresponding characteristic function is
$$ \phi ( t _ {1} , t _ {2} ) = \ \int\limits _ { 0 } ^ { 1 } \frac{dF ( \lambda ) }{[ 1 - it _ {1} - it _ {2} - t _ {1} t _ {2} ( 1 - \lambda )] ^ {1 + \gamma } } . $$
If $ F ( \lambda ) $ is such that $ {\mathsf P} \{ \lambda = R \} = 1 $, then $ c _ {k} = R ^ {k} $, $ \phi ( t _ {1} , t _ {2} ) = [ 1 - it _ {1} - it _ {2} - t _ {1} t _ {2} ( 1 - R)] ^ {- 1- \gamma } $, and $ R $ is the correlation coefficient between $ X _ {1} $ and $ X _ {2} $( $ 0 \leq R \leq 1 $). In this last case the density series can be summed using the formula (cf. [2]):
$$ p ( x _ {1} , x _ {2} ) = \ \frac{( x _ {1} x _ {2} ) ^ \gamma e ^ {- x _ {1} - x _ {2} } }{\Gamma ^ {2} ( \gamma + 1) } \sum _ {k = 0 } ^ \infty R ^ {k} L _ {k} ^ \gamma ( x _ {1} ) L _ {k} ^ \gamma ( x _ {2} ) = $$
$$ = \ \frac{e ^ {- ( x _ {1} + x _ {2} ) / ( 1 - R) } }{( 1 - R) \Gamma ( \gamma + 1) } \left ( \frac{x _ {1} x _ {2} }{R } \right ) ^ {\gamma / 2 } I _ \gamma \left ( \frac{2 \sqrt {x _ {1} x _ {2} R } }{1 - R } \right ) , $$
where $ I _ \gamma $ is the Bessel function of an imaginary argument [2].
References
[1] | I.O. Sarmanov, Trudy Gidrologichesk. Inst. , 162 (1969) pp. 37–61 |
[2] | W. Myller-Lebedeff, "Die Theorie der Integralgleichungen in Anwendung auf einige Reihenentwicklungen" Math. Ann. , 64 (1907) pp. 388–416 |
Comments
This bivariate distribution is just one of the many possible multivariate generalizations of the (univariate) gamma-distribution. See [a1], Chapt. 40 for a survey as well as more details on this one.
References
[a1] | N.L. Johnson, S. Kotz, "Distributions in statistics" , 2. Continuous multivariate distributions , Wiley (1972) |
Gamma-correlation. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Gamma-correlation&oldid=18680