| LrdModelling | R Documentation | 
A collection and description of functions to investigate the long 
range dependence or long memory behavior of an univariate time 
series process. Included are functions to simulate fractional 
Gaussian noise and fractional ARMA processes, and functions to 
estimate the Hurst exponent by several different methods.
The Functions and methods are:
Functions to simulate long memory time series processes:
| fnmSim | Simulates fractional Brownian motion, | 
| - mvn | from the numerical approximation of the stochastic integral, | 
| - chol | from the Choleski's decomposition of the covariance matrix, | 
| - lev | using the method of Levinson, | 
| - circ | using the method of Wood and Chan, | 
| - wave | using the wavelet synthesis, | 
| fgnSim | Simulates fractional Gaussian noise, | 
| - beran | using the method of Beran, | 
| - durbin | using the method Durbin and Levinson, | 
| - paxson | using the method of Paxson, | 
| farimaSim | simulates FARIMA time series processes. | 
Functions to estimate the Hurst exponent:
| aggvarFit | Aggregated variance method, | 
| diffvarFit | Differenced aggregated variance method, | 
| absvalFit | aggregated absolute value (moment) method, | 
| higuchiFit | Higuchi's or fractal dimension method, | 
| pengFit | Peng's or variance of residuals method, | 
| rsFit | R/S Rescaled Range Statistic method, | 
| perFit | periodogram method, | 
| boxperFit | boxed (modified) periodogram method, | 
| hurstSlider | Interactive Display of Hurst Estimates. | 
Function for the wavelet estimator:
| waveletFit | wavelet estimator. | 
fbmSim(n = 100, H = 0.7, method = c("mvn", "chol", "lev", "circ", "wave"),
    waveJ = 7, doplot = TRUE, fgn = FALSE)
fgnSim(n = 1000, H = 0.7, method = c("beran", "durbin", "paxson"))
farimaSim(n = 1000, model = list(ar = c(0.5, -0.5), d = 0.3, ma = 0.1),
    method = c("freq", "time"), ...) 
   
aggvarFit(x, levels = 50, minnpts = 3, cut.off = 10^c(0.7, 2.5), 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL)    
diffvarFit(x, levels = 50, minnpts = 3, cut.off = 10^c(0.7, 2.5), 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL) 
absvalFit(x, levels = 50, minnpts = 3, cut.off = 10^c(0.7, 2.5), moment = 1, 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL) 
higuchiFit(x, levels = 50, minnpts = 2, cut.off = 10^c(0.7, 2.5), 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL)
pengFit(x, levels = 50, minnpts = 3, cut.off = 10^c(0.7, 2.5), 
    method = c("mean", "median"), 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL)
rsFit(x, levels = 50, minnpts = 3, cut.off = 10^c(0.7, 2.5), 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL)
perFit(x, cut.off = 0.1, method = c("per", "cumper"), 
    doplot = FALSE, title = NULL, description = NULL)
boxperFit(x, nbox = 100, cut.off = 0.10, 
    doplot = FALSE, trace = FALSE, title = NULL, description = NULL)      
hurstSlider(x = fgnSim())
  
waveletFit(x, length = NULL, order = 2, octave = c(2, 8), 
    doplot = FALSE, title = NULL, description = NULL)
        
## S4 method for signature 'fHURST'
show(object)
| cut.off | [*Fit] -  | 
| description | [*Fit] -  | 
| doplot | [*Fit] -  | 
| fgn | [fbmSim] -  | 
| H | [fgnSim] -  | 
| length | [waveletFit] -  | 
| levels | [*Fit] -  | 
| method | [fbmSim] -  | 
| minnpts | [*Fit] -  | 
| model | a list with model parameters  | 
| moment | [absvalHurst] -  | 
| n | [fgnSim][farimaSim] -  | 
| nbox | [boxperFit] -  | 
| object | an object of class  | 
| octave | [waveletFit] -  | 
| order | [waveletFit] -  | 
| title | a character string which allows for a project title. | 
| trace | a logical value, by defaul FALSE. Should the estimation process be traced? | 
| waveJ | [fbmSim] -  | 
| x | [*Fit] -  | 
| ... | arguments to be passed. | 
Functions to Simulate Long Memory Processes:
Fractional Gaussian Noise:
The function fgnSim simulates a series of fractional
Gaussian noise, FGN. FGN provides a parsimonious model for 
stationary increments of a self-similar process parameterised 
by the Hurst exponent H and variance. Fractional Gaussian noise 
with H < 0.5 demonstrates negatively autocorrelated or 
anti-persistent behaviour, and FGN with H > 0.5 demonstrates 
1/f , long memory or persistent behaviour, and the special 
case. The case H = 0.5 corresponds to the classical Gaussian 
white noise. One can select from three different 
methods. The first generator named "beran" uses
the fast Fourier transform to generate the series based on 
SPLUS code written originally by J. Beran [1994]. The second
generator named "durbin" produces a FGN series by 
using the Durbin-Levinson coefficients. The algorithm was
reimplemented in pure S based on the C source code written by
V. Teverovsky [199x]. The third generator named 
"paxson" was proposed by V. Paxson [199x], this
approaximate method is a very fast and requires low storage. 
However, the algorithm reveals some weakness in the method
which was discussed by D.A. Rolls [2001].
Fractional ARIMA Processes:
The function farimaSim is a generator for fractional
ARIMA time series processes. A Gaussian FARIMA(0,d,0) series
can be created, where d  is related to the the Hurst 
exponent H through d=H-0.5. This is a particular 
case of the more general Gaussian FARIMA(p,d,q) process which 
follows the same asymptotic relations for their autocovariance 
and the spectral density as do the Gaussian FARIMA(0,d,0) 
processes. Two different generators are implement in S. The 
first named "freq" works in the frequence domain and 
generates the series from the fast Fourier transform based on 
SPLUS code written originally by J. Beran [1994]. The second 
method creates the series in the time domain, therefore named 
"time". The algorithm was reimplemented in pure S based 
on the Fortran source code from the R's fracdiff package 
originally written by C. Fraley [1991]. Details for the algorithm 
are given in J Haslett and A.E. Raftery [1989]. 
Functions to Estimate the Hurst Exponent:
These are 9 functions as described by M.S. Taqqu, V. Teverovsky,
and W. Willinger [1995] to estimate the self similarity parameter 
and/or the intensity of long-range dependence in a time series.
Aggregated Variance Method:
The function aggvarFit computes the Hurst exponent from 
the variance of an aggregated FGN or FARIMA time series process. 
The original time series is divided into blocks of size m. 
Then the sample variance within each block is computed. The slope 
beta=2*H-2 from the least square fit of the logarithm of 
the sample variances versus the logarithm of the block sizes 
provides an estimate for the Hurst exponent H. 
Differenced Aggregated Variance Method:
To distinguish jumps and slowly decaying trends which are two
types of non-stationary, from long-range dependence, the function 
diffvarFit differences the sample variances of successive 
blocks. The slope beta=2*H-2 from the least square fit of 
the logarithm of the differenced sample variances versus the 
logarithm of the block sizes provides an estimate for the Hurst 
exponent H. 
Aggregated Absolute Value/Moment Method:
The function absvalFit computes the Hurst exponent from
the moments moment=M of absolute values of an aggregated 
FGN or FARIMA time series process. The first moment M=1
coincides with the absolute value method, and the second moment 
M=2 with the aggregated variance method. Again, the slope 
beta=M*(H-1) of the regression line of the logarithm of 
the statistic versus the logarithm of the block sizes provides 
an estimate for the Hurst exponent H. 
Higuchi or Fractal Dimension Method:
The function higuchiFit implements a technique which is 
very similar to the absolute value method. Instead of blocks a 
sliding window is used to compute the aggregated series. The 
function involves the calculation the calculation of the length 
of a path and, in principle, finding its fractal Dimension D. 
The slope D=2-H from the least square fit of the logarithm 
of the expected path lengths versus the logarithm of the block 
(window) sizes provides an estimate for the Hurst exponent H. 
Peng or Variance of Residuals Method:
The function pengFit uses the method described by peng.
In Peng's variance of residuals method the series is also divided
into blocks of size m. Within each block the cumulated
sums are computed up to t and a least-squares line 
a+b*t is fitted to the cumulated sums. Then the sample 
variance of the residuals is computed which is proportional to
m^(2*H). The "mean" or "median" are
computed over the blocks. The slope beta=2*H from the 
least square provides an estimate for the Hurst exponent H. 
The R/S Method:
The function rsFit implements the algorithm named 
rescaled range analysis which is dicussed for example 
in detail by B. Mandelbrot and Wallis [199x], B. Mandelbrot [199x] 
and B. Mandelbrot and M.S. Taqqu [199x].
The Periodogram Method:
The function perFit estimates the Hurst exponent from the
periodogram. In the finite variance case, the periodogram is an
estimator of the spectral density of the time series. A series
with long range dependence will show a spectral density with a
lower law behavior in the frequency. Thus, we expect that a
log-log plot of the periodogram versus frequency will display
a straight line, and the slopw can be computed as 1-2H.
In practice one uses only the lowest 10% of the frequencies, 
since the power law behavior holds only for frequencies close to
zero. Varying this cut off may provide additional information.
Plotting H versus the cut off, one should select that
cut off where the curve flattens out to estimate H.
This approach can be selected by the argument method="per".
Alternatively we can select method="cumper". In this case,
instead of using the periodgram itself, the cmulative periodgram
will be investigated. The slope of the double logarithmic fit
is given by 2-2H. More details can be found in the work
of J. Geweke and S. Porter-Hudak [1983] and in Taqqu [?].
The Boxed or Modified Periodogram Method:
The function boxperFit is a modification of the periodogram
method. The algorithm devides the frequency axis into logarithmically
equally spaced boxes and averages the periodogram values corresponding 
to the frequencies inside the box.
The original functions were written by V. Teverovsky and W. Willinger
for SPLUS calling internal functions written in C. The software can 
be found on M. Taqqu's home page:
http://math.bu.edu/people/murad/
In addition the Whittle estimator uses SPlus functions written 
by J. Beran. They can be found in the appendix of his book or on 
the StatLib server:
http://lib.stat.cmu.edu/S/
Note, all nine R functions and internal utility functions are 
reimplemented entirely in S.
Functions to perform a Wavelet Analysis:
The function waveletFit computes the Discrete Wavelet 
Transform, averages the squares of the coefficients of the transform, 
and then performs a linear regression on the logarithm of the 
average, versus the log of the scale parameter of the transform. 
The result should be directly proportional to H providing
an estimate for the Hurst exponent. 
fgnSim and farimaSim return a numeric vector of length 
n, the FGN or FARIMA series.
*Fit returns an S4 object of class fHURST with the
following slots:
| @call | the function call. | 
| @method | a character string with the selected method string. | 
| @hurst | a list with at least one element, the Hurst exponent named
 | 
| @parameters | a list with a varying number of elements describing the input parameters from the argument list. | 
| @data | a list holding the input data. | 
| @fit | a list object with all information of the fit. | 
| @plot | a list object which holds information to create a plot of the fit. | 
| @title | a character string with the name of the test. | 
| @description | a character string with a brief description of the test. | 
waveletFit
V. Paxson, code as listed in the Appendix of his paper 1995, 
J. Beran, ported by Maechler, code as listed in the Appendix of his Book, 
M.S. Taqqu et al. for the S-Plus and C code concerned with the Hurst exponent, 
C. Fraley for the FARIMA simulation code, 
Guy Nason for the functions from the R package 'wavethresh', 
Diethelm Wuertz for the Rmetrics R-port.
Beran J. (1992); Statistics for Long-Memory Processes, Chapman and Hall, New York, 1994.
Haslett J., Raftery A.E. (1989); Space-Time Modelling with Long-Memory Dependence: Assessing Ireland's Wind Power Resource, Applied Statistics 38, pp. 1–50.
Paxson V. (1995); Fast Approximation of Self-Similar Network Traffic, Technical report, LBL-36750/UC-405, Berkeley, and Computer Communcation Review27, p.5–18, 1997.
Rolls D.A. (2001); Improved Fast Approximate Synthesis of Fractional Gaussian Noise, Thesis, Department of Mathematics and Statistics, Queen's University at Kingston, Kingston, Ontario, Canada, 5 pages.
Taqqu M., et al. Hurst Exponent, Several Preprints.
## fgnSim -
   par(mfrow = c(3, 1), cex = 0.75)  
   
   # Beran's Method:
   plot(fgnSim(n = 200, H = 0.75), type = "l",  
     ylim = c(-3, 3), xlab = "time", ylab = "x(t)", main = "Beran")
   
   # Durbin's Method:
   plot(fgnSim(n = 200, H = 0.75, method = "durbin"), type = "l",
     ylim = c(-3, 3), xlab = "time", ylab = "x(t)", main = "Durbin")
   
   # Paxson's Method:
   plot(fgnSim(n = 200, H = 0.75, method = "paxson"), type = "l",
     ylim = c(-3, 3), xlab = "time", ylab = "x(t)", main = "Paxson")
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