What is the name of the function $D(a,x) = fracx^a e^-xGamma(a+1)$?

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Does the function $dfracx^a e^-xGamma(a+1)$ have its own specific name?




Temme [1] introduced the function in (3.1)
$$D(a,x) = fracx^a e^-xGamma(a+1).$$ It is the dominant part in many representations of the incomplete gamma functions (his corresponding Algol function is named dax).



Earlier DiDonato and Morris [2] called it $R(a,x)$.



A closely related function is called regularised_gamma_prefix in the Boost library.



I did not find a 'name' for this function. Are there more known references to it?




[1] N.M. Temme, A Set of Algorithms for the Incomplete Gamma Functions, Probability
in the Engineering and Informational Sciences, 8 (1994), pp. 291-307. Available as
https://ir.cwi.nl/pub/10080/10080D.pdf



[2] A.R. DiDonato, A.H. Morris, Computation of the Incomplete Gamma Function
Ratios and their Inverse. ACM TOMS, Vol 12, No 4, Dec 1986, pp. 377-393.







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    Gamma PDF with parameters $(a+1,1)$.
    – Did
    Jul 27 at 16:24














up vote
5
down vote

favorite
1













Does the function $dfracx^a e^-xGamma(a+1)$ have its own specific name?




Temme [1] introduced the function in (3.1)
$$D(a,x) = fracx^a e^-xGamma(a+1).$$ It is the dominant part in many representations of the incomplete gamma functions (his corresponding Algol function is named dax).



Earlier DiDonato and Morris [2] called it $R(a,x)$.



A closely related function is called regularised_gamma_prefix in the Boost library.



I did not find a 'name' for this function. Are there more known references to it?




[1] N.M. Temme, A Set of Algorithms for the Incomplete Gamma Functions, Probability
in the Engineering and Informational Sciences, 8 (1994), pp. 291-307. Available as
https://ir.cwi.nl/pub/10080/10080D.pdf



[2] A.R. DiDonato, A.H. Morris, Computation of the Incomplete Gamma Function
Ratios and their Inverse. ACM TOMS, Vol 12, No 4, Dec 1986, pp. 377-393.







share|cite|improve this question

















  • 1




    Gamma PDF with parameters $(a+1,1)$.
    – Did
    Jul 27 at 16:24












up vote
5
down vote

favorite
1









up vote
5
down vote

favorite
1






1






Does the function $dfracx^a e^-xGamma(a+1)$ have its own specific name?




Temme [1] introduced the function in (3.1)
$$D(a,x) = fracx^a e^-xGamma(a+1).$$ It is the dominant part in many representations of the incomplete gamma functions (his corresponding Algol function is named dax).



Earlier DiDonato and Morris [2] called it $R(a,x)$.



A closely related function is called regularised_gamma_prefix in the Boost library.



I did not find a 'name' for this function. Are there more known references to it?




[1] N.M. Temme, A Set of Algorithms for the Incomplete Gamma Functions, Probability
in the Engineering and Informational Sciences, 8 (1994), pp. 291-307. Available as
https://ir.cwi.nl/pub/10080/10080D.pdf



[2] A.R. DiDonato, A.H. Morris, Computation of the Incomplete Gamma Function
Ratios and their Inverse. ACM TOMS, Vol 12, No 4, Dec 1986, pp. 377-393.







share|cite|improve this question














Does the function $dfracx^a e^-xGamma(a+1)$ have its own specific name?




Temme [1] introduced the function in (3.1)
$$D(a,x) = fracx^a e^-xGamma(a+1).$$ It is the dominant part in many representations of the incomplete gamma functions (his corresponding Algol function is named dax).



Earlier DiDonato and Morris [2] called it $R(a,x)$.



A closely related function is called regularised_gamma_prefix in the Boost library.



I did not find a 'name' for this function. Are there more known references to it?




[1] N.M. Temme, A Set of Algorithms for the Incomplete Gamma Functions, Probability
in the Engineering and Informational Sciences, 8 (1994), pp. 291-307. Available as
https://ir.cwi.nl/pub/10080/10080D.pdf



[2] A.R. DiDonato, A.H. Morris, Computation of the Incomplete Gamma Function
Ratios and their Inverse. ACM TOMS, Vol 12, No 4, Dec 1986, pp. 377-393.









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edited Jul 27 at 16:06
























asked Jul 27 at 15:57









gammatester

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  • 1




    Gamma PDF with parameters $(a+1,1)$.
    – Did
    Jul 27 at 16:24












  • 1




    Gamma PDF with parameters $(a+1,1)$.
    – Did
    Jul 27 at 16:24







1




1




Gamma PDF with parameters $(a+1,1)$.
– Did
Jul 27 at 16:24




Gamma PDF with parameters $(a+1,1)$.
– Did
Jul 27 at 16:24










1 Answer
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You may see it called the probability density function of a gamma distribution. That is the restriction of this function to the interval $[0,+infty).$ This distribution is that of the sum of $a+1$ independent random variables each of which is exponentially distributed, so that the probability of its being greater than $x$ is $e^-x$ for $xge0.$



One more often sees it written as $dfracx^alpha-1 e^-xGamma(alpha).$ That way $alpha$ is the number of exponentially distributed random variables that are added.



Among those probability distributions called gamma distributions one also finds instances in which a scale parameter is present, thus:
$$
frac left( x/mu right)^alpha-1 e^-x/mu Gamma(alpha) left( frac dx muright) text for xge0. tag$mu$
$$
Sometimes it is parametrized using the reciprocal of the scale parameter, $lambda= dfrac 1 mu:$
$$
frac(lambda x)^alpha-1 e^-lambda xGamma(alpha) (lambda , dx). tag$lambda$
$$



It may be that $alpha$ is not a positive integer, in which case the statement about the sum of $alpha$ random variables may seem not to make sense. But suppose $X_1,X_2$ are independent random variables with
$$
Pr(X_iin A) = int_A fracx^alpha_i-1 e^-xGamma(alpha_i) , dx quad textfor measurable A subseteq [0,+infty), quad i=1,2.
$$
In that case, one has
$$
Pr(X_1+X_2in A) = int_A fracx^alpha_1+alpha_2-1 e^-xGamma(alpha_1+alpha_2) , dx quad textfor measurable A subseteq [0,+infty).
$$
This last probability density function is the convolution of those corresponding to $alpha_1$ and $alpha_2.$ Thus putting $alpha-1$ in the exponent rather than $alpha$ makes this a convolution semigroup in which convolution of these functions corresponds to addition of $alpha$s.



When it's written in the $(lambda)$ form rather than the $mu$ form and $x$ is time in a Poisson process, then $lambda x$ is the average number of arrivals in a time interval of length $x.$ When it's written in the $(mu)$ form, then $mu$ is the average time until the next arrival.






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    1 Answer
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    active

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    1 Answer
    1






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    active

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    up vote
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    accepted










    You may see it called the probability density function of a gamma distribution. That is the restriction of this function to the interval $[0,+infty).$ This distribution is that of the sum of $a+1$ independent random variables each of which is exponentially distributed, so that the probability of its being greater than $x$ is $e^-x$ for $xge0.$



    One more often sees it written as $dfracx^alpha-1 e^-xGamma(alpha).$ That way $alpha$ is the number of exponentially distributed random variables that are added.



    Among those probability distributions called gamma distributions one also finds instances in which a scale parameter is present, thus:
    $$
    frac left( x/mu right)^alpha-1 e^-x/mu Gamma(alpha) left( frac dx muright) text for xge0. tag$mu$
    $$
    Sometimes it is parametrized using the reciprocal of the scale parameter, $lambda= dfrac 1 mu:$
    $$
    frac(lambda x)^alpha-1 e^-lambda xGamma(alpha) (lambda , dx). tag$lambda$
    $$



    It may be that $alpha$ is not a positive integer, in which case the statement about the sum of $alpha$ random variables may seem not to make sense. But suppose $X_1,X_2$ are independent random variables with
    $$
    Pr(X_iin A) = int_A fracx^alpha_i-1 e^-xGamma(alpha_i) , dx quad textfor measurable A subseteq [0,+infty), quad i=1,2.
    $$
    In that case, one has
    $$
    Pr(X_1+X_2in A) = int_A fracx^alpha_1+alpha_2-1 e^-xGamma(alpha_1+alpha_2) , dx quad textfor measurable A subseteq [0,+infty).
    $$
    This last probability density function is the convolution of those corresponding to $alpha_1$ and $alpha_2.$ Thus putting $alpha-1$ in the exponent rather than $alpha$ makes this a convolution semigroup in which convolution of these functions corresponds to addition of $alpha$s.



    When it's written in the $(lambda)$ form rather than the $mu$ form and $x$ is time in a Poisson process, then $lambda x$ is the average number of arrivals in a time interval of length $x.$ When it's written in the $(mu)$ form, then $mu$ is the average time until the next arrival.






    share|cite|improve this answer



























      up vote
      5
      down vote



      accepted










      You may see it called the probability density function of a gamma distribution. That is the restriction of this function to the interval $[0,+infty).$ This distribution is that of the sum of $a+1$ independent random variables each of which is exponentially distributed, so that the probability of its being greater than $x$ is $e^-x$ for $xge0.$



      One more often sees it written as $dfracx^alpha-1 e^-xGamma(alpha).$ That way $alpha$ is the number of exponentially distributed random variables that are added.



      Among those probability distributions called gamma distributions one also finds instances in which a scale parameter is present, thus:
      $$
      frac left( x/mu right)^alpha-1 e^-x/mu Gamma(alpha) left( frac dx muright) text for xge0. tag$mu$
      $$
      Sometimes it is parametrized using the reciprocal of the scale parameter, $lambda= dfrac 1 mu:$
      $$
      frac(lambda x)^alpha-1 e^-lambda xGamma(alpha) (lambda , dx). tag$lambda$
      $$



      It may be that $alpha$ is not a positive integer, in which case the statement about the sum of $alpha$ random variables may seem not to make sense. But suppose $X_1,X_2$ are independent random variables with
      $$
      Pr(X_iin A) = int_A fracx^alpha_i-1 e^-xGamma(alpha_i) , dx quad textfor measurable A subseteq [0,+infty), quad i=1,2.
      $$
      In that case, one has
      $$
      Pr(X_1+X_2in A) = int_A fracx^alpha_1+alpha_2-1 e^-xGamma(alpha_1+alpha_2) , dx quad textfor measurable A subseteq [0,+infty).
      $$
      This last probability density function is the convolution of those corresponding to $alpha_1$ and $alpha_2.$ Thus putting $alpha-1$ in the exponent rather than $alpha$ makes this a convolution semigroup in which convolution of these functions corresponds to addition of $alpha$s.



      When it's written in the $(lambda)$ form rather than the $mu$ form and $x$ is time in a Poisson process, then $lambda x$ is the average number of arrivals in a time interval of length $x.$ When it's written in the $(mu)$ form, then $mu$ is the average time until the next arrival.






      share|cite|improve this answer

























        up vote
        5
        down vote



        accepted







        up vote
        5
        down vote



        accepted






        You may see it called the probability density function of a gamma distribution. That is the restriction of this function to the interval $[0,+infty).$ This distribution is that of the sum of $a+1$ independent random variables each of which is exponentially distributed, so that the probability of its being greater than $x$ is $e^-x$ for $xge0.$



        One more often sees it written as $dfracx^alpha-1 e^-xGamma(alpha).$ That way $alpha$ is the number of exponentially distributed random variables that are added.



        Among those probability distributions called gamma distributions one also finds instances in which a scale parameter is present, thus:
        $$
        frac left( x/mu right)^alpha-1 e^-x/mu Gamma(alpha) left( frac dx muright) text for xge0. tag$mu$
        $$
        Sometimes it is parametrized using the reciprocal of the scale parameter, $lambda= dfrac 1 mu:$
        $$
        frac(lambda x)^alpha-1 e^-lambda xGamma(alpha) (lambda , dx). tag$lambda$
        $$



        It may be that $alpha$ is not a positive integer, in which case the statement about the sum of $alpha$ random variables may seem not to make sense. But suppose $X_1,X_2$ are independent random variables with
        $$
        Pr(X_iin A) = int_A fracx^alpha_i-1 e^-xGamma(alpha_i) , dx quad textfor measurable A subseteq [0,+infty), quad i=1,2.
        $$
        In that case, one has
        $$
        Pr(X_1+X_2in A) = int_A fracx^alpha_1+alpha_2-1 e^-xGamma(alpha_1+alpha_2) , dx quad textfor measurable A subseteq [0,+infty).
        $$
        This last probability density function is the convolution of those corresponding to $alpha_1$ and $alpha_2.$ Thus putting $alpha-1$ in the exponent rather than $alpha$ makes this a convolution semigroup in which convolution of these functions corresponds to addition of $alpha$s.



        When it's written in the $(lambda)$ form rather than the $mu$ form and $x$ is time in a Poisson process, then $lambda x$ is the average number of arrivals in a time interval of length $x.$ When it's written in the $(mu)$ form, then $mu$ is the average time until the next arrival.






        share|cite|improve this answer















        You may see it called the probability density function of a gamma distribution. That is the restriction of this function to the interval $[0,+infty).$ This distribution is that of the sum of $a+1$ independent random variables each of which is exponentially distributed, so that the probability of its being greater than $x$ is $e^-x$ for $xge0.$



        One more often sees it written as $dfracx^alpha-1 e^-xGamma(alpha).$ That way $alpha$ is the number of exponentially distributed random variables that are added.



        Among those probability distributions called gamma distributions one also finds instances in which a scale parameter is present, thus:
        $$
        frac left( x/mu right)^alpha-1 e^-x/mu Gamma(alpha) left( frac dx muright) text for xge0. tag$mu$
        $$
        Sometimes it is parametrized using the reciprocal of the scale parameter, $lambda= dfrac 1 mu:$
        $$
        frac(lambda x)^alpha-1 e^-lambda xGamma(alpha) (lambda , dx). tag$lambda$
        $$



        It may be that $alpha$ is not a positive integer, in which case the statement about the sum of $alpha$ random variables may seem not to make sense. But suppose $X_1,X_2$ are independent random variables with
        $$
        Pr(X_iin A) = int_A fracx^alpha_i-1 e^-xGamma(alpha_i) , dx quad textfor measurable A subseteq [0,+infty), quad i=1,2.
        $$
        In that case, one has
        $$
        Pr(X_1+X_2in A) = int_A fracx^alpha_1+alpha_2-1 e^-xGamma(alpha_1+alpha_2) , dx quad textfor measurable A subseteq [0,+infty).
        $$
        This last probability density function is the convolution of those corresponding to $alpha_1$ and $alpha_2.$ Thus putting $alpha-1$ in the exponent rather than $alpha$ makes this a convolution semigroup in which convolution of these functions corresponds to addition of $alpha$s.



        When it's written in the $(lambda)$ form rather than the $mu$ form and $x$ is time in a Poisson process, then $lambda x$ is the average number of arrivals in a time interval of length $x.$ When it's written in the $(mu)$ form, then $mu$ is the average time until the next arrival.







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        share|cite|improve this answer



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        edited Jul 27 at 16:25


























        answered Jul 27 at 16:12









        Michael Hardy

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