the value of xi such that the variance is
var(Y) = phi * mu^xi
power
a synonym for xi
mu
the mean
phi
the dispersion
exact
logical flag;
if TRUE (the default),
exact zeros are used with
the W-algorithm of Sidi (1982);
if FALSE,
approximate (asymptotic) zeros are used in place of exact zeros.
Using asymptotic zeros requires less computation but is often less accurate;
using exact zeros can be slower but generally improves accuracy.
method
either 1, 2 or 3,
determining which of three methods to use to compute the density
using the inversion method.
If method is NULL (the default),
the optimal method (in terms of relative accuracy) is used, element-by-element of y.
See the Note in the Details section below
Details
The Tweedie family of distributions belong to the class
of exponential dispersion models (EDMs),
famous for their role in generalized linear models.
The Tweedie distributions are the EDMs with a variance of the form
var(Y) = phi * mu^power
where power is greater than or equal to one, or less than or equal to zero.
This function only evaluates for power
greater than or equal to one.
Special cases include the
normal (power=0),
Poisson (power=1 with phi=1),
gamma (power=2)
and
inverse Gaussian (power=3)
distributions.
For other values of power,
the distributions are still defined but cannot be written in closed form,
and hence evaluation is very difficult.
When 1 < power < 2,
the distribution are continuous for Y greater than zero,
with a positive mass at Y=0.
For power > 2,
the distributions are continuous for Y greater than zero.
This function evaluates the density or cumulative probability
using one of two methods,
depending on the combination of parameters.
One method is the evaluation of an infinite series.
The second interpolates some stored values computed from a
Fourier inversion technique.
The function dtweedie.inversion
evaluates the density using a Fourier series technique;
ptweedie.inversion does likewise for the cumulative
probabilities.
The actual code is contained in an external FORTRAN program.
Different code is used for power > 2
and for 1 < power < 2.
The function dtweedie.series evaluates the density
using a series expansion;
a different series expansion
is used for power > 2 and for 1 < power < 2.
The function ptweedie.series does likewise for the
cumulative probabilities but only for 1 < power < 2.
The function dtweedie.stable exploits the link between
the stable distribution (Nolan, 1997) and Tweedie distributions,
as discussed in Jorgensen, Chapter 4.
These are computed using Nolan's algorithm as implemented
in the stabledist package (which is therefore required to use
the dtweedie.stable function).
The function dtweedie uses a two-dimensional interpolation procedure to
compute the density for some parts of the parameter space from
previously computed values found from the series or the
inversion. For other parts of the parameter space,
the series solution is found.
ptweedie returns either the computed series
solution or inversion solution.
Value
density (dtweedie),
probability (ptweedie),
quantile (qtweedie)
or random sample (rtweedie)
for the given Tweedie distribution with parameters
mu,
phi
and
power.
Note
The methods changed from version 1.4 to 1.5
(methods 1 and 2 swapped).
The methods are defined in Dunn and Smyth (2008).
Dunn, P. K. and Smyth, G. K. (2008).
Evaluation of Tweedie exponential dispersion model densities by Fourier inversion.
Statistics and Computing,
18, 73–86.
Dunn, Peter K and Smyth, Gordon K (2005).
Series evaluation of Tweedie exponential dispersion model densities
Statistics and Computing,
15(4). 267–280.
Dunn, Peter K and Smyth, Gordon K (2001).
Tweedie family densities: methods of evaluation.
Proceedings of the 16th International Workshop on Statistical Modelling,
Odense, Denmark, 2–6 July
Jorgensen, B. (1987).
Exponential dispersion models.
Journal of the Royal Statistical Society, B,
49, 127–162.
Jorgensen, B. (1997).
Theory of Dispersion Models.
Chapman and Hall, London.
Nolan, John P (1997).
Numerical calculation of stable densities and distribution functions.
Communication in Statistics—Stochastic models,
13(4). 759–774.
Sidi, Avram (1982).
The numerical evaluation of very oscillatory infinite integrals by
extrapolation.
Mathematics of Computation38(158), 517–529.
Sidi, Avram (1988).
A user-friendly extrapolation method for
oscillatory infinite integrals.
Mathematics of Computation51(183), 249–266.
Tweedie, M. C. K. (1984).
An index which distinguishes between some important exponential families.
Statistics: Applications and New Directions.
Proceedings of the Indian Statistical Institute Golden Jubilee International Conference
(Eds. J. K. Ghosh and J. Roy), pp. 579-604. Calcutta: Indian Statistical Institute.
See Also
dtweedie.saddle
Examples
### Plot a Tweedie density
power <- 2.5
mu <- 1
phi <- 1
y <- seq(0, 6, length=500)
fy <- dtweedie( y=y, power=power, mu=mu, phi=phi)
plot(y, fy, type="l", lwd=2, ylab="Density")
# Compare to the saddlepoint density
f.saddle <- dtweedie.saddle( y=y, power=power, mu=mu, phi=phi)
lines( y, f.saddle, col=2 )
legend("topright", col=c(1,2), lwd=c(2,1),
legend=c("Actual","Saddlepoint") )
### A histogram of Tweedie random numbers
hist( rtweedie( 1000, power=1.2, mu=1, phi=1) )
### An example of the multimodal feature of the Tweedie
### family with power near 1 (from Dunn and Smyth, 2005).
y <- seq(0.001,2,len=1000)
mu <- 1
phi <- 0.1
p <- 1.02
f1 <- dtweedie(y,mu=mu,phi=phi,power=p)
plot(y, f1, type="l", xlab="y", ylab="Density")
p <- 1.05
f2<- dtweedie(y,mu=mu,phi=phi,power=p)
lines(y,f2, col=2)
### Compare series and saddlepoint methods
y <- seq(0.001,2,len=1000)
mu <- 1
phi <- 0.1
p <- 1.02
f.series <- dtweedie.series( y,mu=mu,phi=phi,power=p )
f.saddle <- dtweedie.saddle( y,mu=mu,phi=phi,power=p )
f.all <- c( f.series, f.saddle )
plot( range(f.all) ~ range( y ), xlab="y", ylab="Density",
type="n")
lines( f.series ~ y, lty=1, col=1)
lines( f.saddle ~ y, lty=3, col=3)
legend("topright", lty=c(1,3), col=c(1,3),
legend=c("Series","Saddlepoint") )