Build all transition probability matrices of an periodic-HSMM-approximating HMM
Build all transition probability matrices of an periodic-HSMM-approximating HMM
Hidden semi-Markov models (HSMMs) are a flexible extension of HMMs. For direct numerical maximum likelhood estimation, HSMMs can be represented as HMMs on an enlarged state space (of size M) and with structured transition probabilities. This function computes the transition matrices of a periodically inhomogeneos HSMMs.
tpm_phsmm2(omega, dm, eps =1e-10)
Arguments
omega: embedded transition probability matrix
Either a matrix of dimension c(N,N) for homogeneous conditional transition probabilities, or an array of dimension c(N,N,L) for inhomogeneous conditional transition probabilities.
dm: state dwell-time distributions arranged in a list of length(N)
Each list element needs to be a matrix of dimension c(L, N_i), where each row t is the (approximate) probability mass function of state i at time t.
eps: rounding value: If an entry of the transition probabily matrix is smaller, than it is rounded to zero.
Returns
array of dimension c(N,N,L), containing the extended-state-space transition probability matrices of the approximating HMM for each time point of the cycle.
Examples
N =3L =24# time-varying mean dwell timesLambda = exp(matrix(rnorm(L*N,2,0.5), nrow = L))sizes = c(25,25,25)# approximating chain with 75 states# state dwell-time distributionsdm = list()for(i in1:3){ dmi = matrix(nrow = L, ncol = sizes[i])for(t in1:L){ dmi[t,]= dpois(1:sizes[i]-1, Lambda[t,i])} dm[[i]]= dmi
}## homogeneous conditional transition probabilites# diagonal elements are zero, rowsums are oneomega = matrix(c(0,0.5,0.5,0.2,0,0.8,0.7,0.3,0), nrow = N, byrow =TRUE)# calculating extended-state-space t.p.m.sGamma = tpm_phsmm(omega, dm)## inhomogeneous conditional transition probabilites# omega can be an arrayomega = array(rep(omega,L), dim = c(N,N,L))omega[1,,4]= c(0,0.2,0.8)# small change for inhomogeneity# calculating extended-state-space t.p.m.sGamma = tpm_phsmm(omega, dm)