#' Inhomogeneous anisotropic pcf function, cylinder version
#'
#' Estimate a cylinder-pcf function for second order reweighted ("inhomogeneous") pattern.
#'
#' @param x pp, list with $x~coordinates $bbox~bounding box
#' @param u unit vector(s) of direction, as row vectors. Default: x and y axis.
#' @param epsilon The cylinder half-width
#' @param r radius vector at which to evaluate the function
#' @param lambda optional vector of intensity estimates at points
#' @param lambda_h if lambda missing, use this bandwidth in a kernel estimate of lambda(x)
#' @param r_h smoothing for range dimension, epanechnikov kernel
#' @param stoyan If r_h not given, use r_h=stoyan/lambda^(1/dim). Same as 'stoyan' in spatstat's pcf.
#' @param renormalise See details.
#' @param border Use translation correction? Default=1, yes. Only for cuboidal windows.
#' @param aspect If given, instead of using a fixed halfwidth (epsilon) take the halfwidth to be r/(2*aspect). Default : 1/3
#' @param ... passed on to e.g. \link{intensity_at_points}
#' @details
#'
#' Computes a second order reweighted version of the cylinder-pcf, defined as the function to integrate in range over [0,R] to get the cylinder-K(R) function.
#'
#' Lambda(x) at points can be given,
#' or else it will be estimated using Epanechnikov kernel smoothing. See
#'
#' If 'renormalise=TRUE', we normalise the lambda estimate so that sum(1/lambda(x))=|W|. This corresponds in \code{spatstat}'s \code{Kinhom} to setting 'normpower=2'.
#'
#' @return
#' Returns a dataframe.
#'
#' @useDynLib Kdirectional
#' @export
pcf_anin_cylinder <- function(x, u, epsilon, r, lambda=NULL, lambda_h, r_h,
stoyan=0.15,
renormalise=TRUE,
border=1,
aspect = 1/3,
...) {
x <- check_pp(x)
bbox <- x$bbox
if(is.bbquad(bbox)) stop("bbquad window not yet supported.")
dim <- ncol(bbox)
V <- bbox_volume(bbox)
# directions
if(missing(u)){
u <- diag(c(1), dim)
}
#
# make sure unit vectors
u <- rbind(u)
u <- t(apply(u, 1, function(ui) ui/c(sqrt(t(ui)%*%ui) )))
#
# ranges
if(missing(r)) {
sidelengths <- apply(bbox, 2, diff)
bl <- min(sidelengths)*0.3
r <- seq(0, bl, length=50)
}
# central half-angle
if(!is.null(aspect)) {
epsilon <- aspect * r / 2
}
else{
if(missing(epsilon)){
stop("cylinder half-width epsilon missing, and no default available.")
}
if(length(epsilon) == 1) epsilon <- rep(epsilon, length(r))
else if( length(epsilon) == length(r)) {}
else stop("epsilon should be length 1 or length(r).")
}
if(any(epsilon < 0)) stop("epsilon should >0")
# check intensity
if(!missing(lambda)){
err <- paste("lambda should be a single positive number or a vector of length", nrow(x$x))
if(!is.vector(lambda)) stop(err)
if(length(lambda) != nrow(x$x)){
if(length(lambda)!= 1) stop(err)
lambda <- rep(lambda, nrow(x$x))
}
}
else{
# estimate lambda
if(missing(lambda_h)) stop("Need lambda_h to estimate the intensity function")
lambda <- intensity_at_points(x, bw=lambda_h, ...)
}
# Check the lambda's positive
if(!all(lambda>0)) stop("Check your parameters. Lambda's need to be positive.")
if(missing(r_h)) {
lambda0 <- nrow(x$x)/V # mean lambda
r_h <- stoyan/lambda0^(1/dim)
}
# if renormalisation of the intensity is in order
if(renormalise) {
S <- V/sum(1/lambda)
normpower <- 2
S <- S^normpower
} else {
S<-1
}
# new, do it in one function
# check divisor
fun <- pcf_anin_cylindrical_c
div <- 1
# Run
coord <- x$x
out <- fun(coord, lambda, bbox, r, r_h, u, epsilon, border)
#
# scaling
#
out <- S * out # double sum
# in case translation weights are not applied
if(border==0) out <- out/V
#
# scale
norm <- pi^((dim-1)/2)/gamma((dim-1)/2+1) * epsilon^(dim-1) * div
out <- out/norm
#
# compile output
# direction names
dir_names <- apply(u, 1, function(ui) paste0("(", paste0(ui, collapse=","), ")" ))
# theoretical
theo <- rep(1, length(r))
#
gest <- data.frame(r=r, theo=theo, out)
names(gest)[] <- c("r", "theo", dir_names)
rownames(gest) <- NULL
attr(gest, "epsilon") <- epsilon
attr(gest, "aspect") <- aspect
attr(gest, "r_h") <- r_h
attr(gest, "fname") <- "pcf_anin_cylinder"
#done
class(gest) <- c("pcf_anin", is(gest))
gest
}
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