Nothing
########################################################################
# Minimax distance
########################################################################
mMdist=function(D,neval=1e5,method="lattice",region="hypercube",const=NA,eval_pts=NA){
bd <- c(0,1) #Default limits are (0,1)
p <- ncol(D)
# Define transformation function
flg <- T #set eval points
switch(region,
hypercube = {
tf <- function(D,by,num_proc){return(D)}
checkBounds <- function(D){ #function for checking bound
return(D)
}
},
simplex = {
tf <- CtoA;
checkBounds <- function(D){ #function for checking bound
return(D)
}
},
ball = {
tf <- CtoB;
bd <- c(-1,1);
checkBounds <- function(D){ #function for checking bound
good.idx <- which(rowSums(D^2)<=1)
return(D[good.idx,])
}
},
ineq = {
tf <- function(D,by,num_proc){ #randomly sample until enough points
num_pts <- nrow(D)
samp <- matrix(NA,nrow=num_pts,ncol=p)
cur_pts <- 0
while (cur_pts < num_pts){
xx <- stats::runif(p)
if (const(xx)){
samp[cur_pts+1,] <- xx
cur_pts <- cur_pts + 1
}
}
return(samp)
}
checkBounds <- function(D){ #function for checking bound
good.idx <- apply(D,1,const)
return(D[good.idx,])
}
},
custom = {
tf <- function(D,by,num_proc){return(D)}
checkBounds <- function(D){ #function for checking bound
return(D)
}
M <- eval_pts
flg <- F
}
)
regionby=ifelse(ncol(D)>2,1e-3,-1)
by <- regionby
# Generating evaluation points
if (flg){
switch(method,
lattice = {
m <- nrow(D)
d <- ncol(D)
M <- tf(as.matrix(Lattice(max(conf.design::primes(neval)),d)),by,parallel::detectCores())
M <- rbind(M,tf(gtools::permutations(3,p,c(0.0,0.5,1.0),repeats.allowed=TRUE))) #add 3^p design
M <- checkBounds(M)
},
sobol = {
m <- nrow(D)
d <- ncol(D)
M <- tf(randtoolbox::sobol(neval,d),by,parallel::detectCores())
M <- rbind(M,tf(gtools::permutations(3,p,c(0.0,0.5,1.0),repeats.allowed=TRUE))) #add 3^p design
M <- checkBounds(M)
}
)
}else{
m <- nrow(D)
d <- ncol(D)
}
# Compute minimax distance
mM=as.matrix(pdist::pdist(M,D))
ind=apply(mM,1,which.min)
distD=numeric(m)
for(i in 1:m){
distD[i]=max(mM[ind==i,i])
}
maxD <- max(distD)
maxI <- which.max(distD)
ptI <- which(ind==maxI)
ptI <- ptI[which.max(mM[ind==maxI,maxI])]
return(list(dist=max(distD),dist.vec=distD,far.pt=M[ptI,],far.despt=D[maxI,]))
}
# ########################################################################
# # Maximin distance
# ########################################################################
#
# Mmdist=function(D){
# distD <- max(stats::dist(D))
# return(distD)
# }
########################################################################
# Computing shifted lattices
########################################################################
Lattice=function(n,p,shift=FALSE){
#n: number of points in the lattice rule, scalar, must be prime
#n = 101
#s_max: number of dimensions, scalar
s_max = p
#omega: function for the varying kernel part of the shift-invariant kernel function (assumed to be symmetric)
omega=function(x)
2*pi^2*(x^2-x+1/6)
#gamma:gamma parameters for AC weighting per dimension, vector of length s_max
gamma = rep(1,s_max) / s_max
#beta: beta parameters for DC weighting per dimension, vector of length s_max
beta = rep(1,s_max)
############################################
#Define fuction "powmod"
#Calculate x^a (mod n) using the Russian Peasant method
powmod=function(x,a,n){
y=1
u=x
while(a>0){
if(a%%2==1)
y=(y*u)%%n
u=(u*u)%%n
a = floor(a / 2)
}
return(y)
}
#Define fuction "generatorp"
#Return a generator for the cyclic group multiplication modulo p
#Also called a primitive root of p
#input:
#p:a prime number
#output:
#g:the generator
#Get all irreducible factors of an integer
generatorp <- function(p){
primef=as.numeric(unique(conf.design::factorize(p-1)))
g=2
i=1
while(i<=length(primef)){
if(powmod(g,(p-1)/primef[i],p)==1){
g=g+1
i=0
}
i=i+1
}
return(g)
}
############################################
###Generate the lattice rule###
#s_max=p
m = (n-1)/2 #assume the omega function symmetric around 1/2
E2 = rep(0,m) # the vector $\tilde{\vec{E}}^2$ in the text
cumbeta = cumprod(beta)
g = generatorp(n) #generator $g$ for $\{1, 2, \ldots, n-1\}$
perm=rep(0,m) #permutation formed by positive powers of $g$
perm[1]=1
for(j in 1:(m-1))
perm[j+1]=(perm[j]*g)%%n
perm = apply(cbind(n - perm, perm),1,min) #map everything back to $[1, n/2)$
psi= apply(matrix(perm/n,ncol=1),1,omega) #the vector $\vec{\psi}'$
psi0 = omega(0) # zero index: $\psi(0)$
fft_psi = stats::fft(psi)
#z:generating vector of the lattice rule, vector of length s_max
#e2:optimal square error per dimension (= one for each iteration), vector of length s_max
z=rep(NA,s_max)
e2=rep(NA,s_max)
q=rep(1,m) #permuted product vector $\vec{q}'$ (without zero index)
q0 = 1 #zero index of permuted product vector: $q(0)$
for(s in 1:s_max){
#step 2a: circulant matrix-vector multiplication
E2=stats::fft(fft_psi*stats::fft(q),inverse=T)/m
E2 = Re(E2)#remove imaginary rounding errors
#step 2b: choose $w_s$ and $z_s$ which give minimal value
min_E2=min(E2)
w=which.min(E2)#pick index of minimal value
if(s==1){
w=1
noise = abs(E2[1] - min_E2)
}
z[s]=perm[w]
#extra: we want to know the exact value of the worst-case error
e2[s] = -cumbeta[s] + ( beta[s] * (q0 + 2*sum(q)) +
gamma[s] * (psi0*q0 + 2*min_E2) ) / n
#step 2c: update $\vec{q}$
q = (beta[s] + gamma[s] * psi[c(seq(w,1,-1),seq(m,(w+1),-1))])* q
q0 = (beta[s] + gamma[s] * psi0) * q0
}
#Output
#z:generating vector of the lattice rule, vector of length s_max
#e2:optimal square error per dimension (= one for each iteration), vector of length s_max
#output=data.frame(z,e2,sqrt(e2))
tseq=function(gamma)
{
x=((((1:n))*gamma)%%n)/n
return(x)
}
D=matrix(0,nrow=n,ncol=p)
for(i in 1:p)
D[,i]=cbind(tseq(z[i]))
l=apply(D,2,min)
u=apply(D,2,max)
D=.5/n+(1-1/n)*(D-rep(1,n)%*%t(l))/(rep(1,n)%*%t(u-l))
if (shift){ # random shift
D <- apply(D,2,function(xx){ ((xx+stats::runif(1))%%1) })
}
return(D)
}
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