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#' Poincare map
#' @description
#' Computes the Poincare map of the reconstructed trajectories in the phase-space.
#' @description
#' The Poincare map is a classical dynamical system technique that replaces the
#' n-th dimensional trajectory in the phase space with an (n-1)-th order discrete-time
#' called the Poincare map. The points of the Poincare map are the intersection of
#' the trajectories in the phase-space with a certain Hyper-plane.
#' @details
#' This function computes the Poincare map taking the Takens' vectors as the continuous trajectory
#' in the phase space. The \emph{takens} param has been included so that the user may
#' specify the real phase-space instead of using the phase-space reconstruction (see
#' examples).
#' @param time.series The original time series from which the phase-space reconstruction is done.
#' @param embedding.dim Integer denoting the dimension in which we shall embed the \emph{time.series}.
#' @param time.lag Integer denoting the number of time steps that will be use to construct the
#' Takens' vectors.
#' @param takens Instead of specifying the \emph{time.series}, the \emph{embedding.dim} and the \emph{time.lag}, the user
#' may specify directly the Takens' vectors.
#' @param normal.hiperplane.vector The normal vector of the hyperplane that will be used to compute the Poincare map. If
#' the vector is not specifyed the program choses the vector (0,0,...,1).
#' @param hiperplane.point A point on the hyperplane (an hyperplane is defined with a point and a normal vector).
#' @return Since there are three different Poincare maps, an R list is returned storing all the information
#' related which all of these maps:
#' \itemize{
#' \item The positive Poincare map is formed by all the intersections with the hyperplane in positive direction
#' (defined by the normal vector). The \emph{pm.pos} returns the points of the map whereas that \emph{pm.pos.time} returns
#' the number of time steps since the beggining where the intersections occurred.
#' \item Similarly we define a negative Poincare map (\emph{pm.neg} and \emph{pm.neg.time}).
#' \item Finally, we may define a two-side Poincare map that stores all the intersections (no matter the direction
#' of the intersection) (\emph{pm} and \emph{pm.time}).
#' }
#' @examples
#' \dontrun{
#' r=rossler(a = 0.2, b = 0.2, c = 5.7, start=c(-2, -10, 0.2),
#' time=seq(0,300,by = 0.01), do.plot=FALSE)
#' takens=cbind(r$x,r$y,r$z)
#' # calculate poincare sections
#' pm=poincareMap(takens = takens,normal.hiperplane.vector = c(0,1,0),
#' hiperplane.point=c(0,0,0) )
#' plot3d(takens,size=0.7)
#' points3d(pm$pm,col="red")}
#' @references Parker, T. S., L. O. Chua, and T. S. Parker (1989). Practical
#' numerical algorithms for chaotic systems. Springer New York
#' @author Constantino A. Garcia
#' @rdname poincareMap
#' @export poincareMap
#' @useDynLib nonlinearAnalysis
poincareMap=function(time.series=NULL, embedding.dim=2, time.lag=1, takens = NULL, normal.hiperplane.vector = NULL, hiperplane.point ){
if (is.null(takens)){takens = buildTakens(time.series,embedding.dim,time.lag)}
dimension = ncol(takens)
n.points = nrow(takens)
if (is.null(normal.hiperplane.vector)){
normal.hiperplane.vector = rep(0,dimension)
normal.hiperplane.vector[[dimension]] = 1
hiperplane.point = rep(0,dimension)
}
if (length(normal.hiperplane.vector) != dimension){
stop("The hiperplane was defined in a wrong dimensional space\n")
}
# this variables will store information about the poincare map
poincare.map.series = matrix(0,nrow=n.points,ncol=dimension)
positive.poincare.map.series = matrix(0,nrow=n.points,ncol=dimension)
negative.poincare.map.series = matrix(0,nrow=n.points,ncol=dimension)
crossing.time = rep(0,n.points)
positive.crossing.time = rep(0,n.points)
negative.crossing.time = rep(0,n.points)
number.of.crossings = 0
number.of.positive.crossings = 0
number.of.negative.crossings = 0
poincare = .C("poincareMap", timeSeries = as.double(takens),
nPoints = as.integer(n.points), dimension = as.integer(dimension),
poincareMapSeries = as.double(poincare.map.series),
positivePoincareMapSeries = as.double(positive.poincare.map.series),
negativePoincareMapSeries = as.double(negative.poincare.map.series),
crossingTime = as.double(crossing.time),
positiveCrossingTime = as.double(positive.crossing.time),
negativeCrossingTime = as.double(negative.crossing.time),
numberCrossings = as.integer(number.of.crossings),
numberPositiveCrossings = as.integer(number.of.positive.crossings),
numberNegativeCrossings = as.integer(number.of.negative.crossings),
hiperplanePoint = as.double(hiperplane.point),
normalVector = as.double(normal.hiperplane.vector),
PACKAGE="nonlinearAnalysis")
# arranging data to return it
poincare.map.series = matrix(poincare$poincareMapSeries,nrow=n.points,ncol=dimension)
poincare.map.series = poincare.map.series[1:poincare$numberCrossings,]
positive.poincare.map.series = matrix(poincare$positivePoincareMapSeries,nrow=n.points,ncol=dimension)
positive.poincare.map.series = positive.poincare.map.series[1:poincare$numberPositiveCrossings,]
negative.poincare.map.series = matrix(poincare$negativePoincareMapSeries,nrow=n.points,ncol=dimension)
negative.poincare.map.series = negative.poincare.map.series[1:poincare$numberNegativeCrossings,]
return(list(pm = poincare.map.series, pm.time = poincare$crossingTime[1:poincare$numberCrossings],
pm.pos = positive.poincare.map.series, pm.pos.time = poincare$positiveCrossingTime[1:poincare$numberPositiveCrossings],
pm.neg = negative.poincare.map.series, pm.neg.time = poincare$negativeCrossingTime[1:poincare$numberNegativeCrossings]))
}
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