Outer-grid posterior covariance of a joint fit's latent coordinates
Source:R/nested_laplace_joint_helpers.R
tulpa_joint_inner_vcov_mixture.RdThe law-of-total-covariance mixture over the outer grid,
$$V = \sum_k w_k [C_k + (m_k - \bar m)(m_k - \bar m)^T],$$
with C_k the same per-cell constrained block
tulpa_joint_inner_vcov_blocks() returns, accumulated inside the engine
without holding one block per cell. Memory is one length(idx) square
result whatever the grid size, so this is the door for an idx that
carries a field.
Usage
tulpa_joint_inner_vcov_mixture(
Q_p_per_grid,
Q_i_per_grid,
Q_x_per_grid,
n_x,
idx,
n_dense,
A_cols_list,
weights,
modes = NULL,
field_marginal = TRUE,
n_threads = 1L
)Arguments
- Q_p_per_grid, Q_i_per_grid, Q_x_per_grid
Per-outer-grid-cell CSC storage of the latent precision
Q(fit$Q_csc_p_per_grid/_i_per_grid/_x_per_grid), one list element per cell.- n_x
Integer, the latent dimension
Qis built over (fit$Q_csc_n).- idx
Integer vector (1-based) of latent coordinates to extract the sub-block for.
- n_dense
Integer, the number of leading
idxentries that are dense fixed effects rather than field coordinates (see Details).- A_cols_list
A list of integer vectors, one per sum-to-zero constraint group, each the (1-based) latent coordinates that group averages to zero.
- weights
Numeric, one non-negative weight per outer-grid cell (normalized here). A cell of zero weight is never extracted.
- modes
Optional
n_grid x length(idx)matrix of the cell modes onidx.NULLreturns the within-cell term alone.- field_marginal
Logical; if
TRUE(default) andn_dense < length(idx), only the field coordinates' marginal variances are computed (a single Takahashi pass) rather than their full dense sub-block.- n_threads
Integer, grid cells processed concurrently.
Value
A list: vcov, the mixture covariance; mean, the weighted mean
of modes (NULL without them); dense_blocks, one
n_dense x n_dense block per cell (NULL where the cell was not
extracted); failed, the cells of positive weight whose block is
missing (no stored precision, or its Cholesky failed). Such a cell keeps
its weight and contributes its between-cell term only. With
field_marginal = TRUE the field x field part of the within term is its
diagonal.
Examples
# Two outer-grid cells of a latent precision over two fixed effects and a
# ten-node random-walk field (sum-to-zero), each stored as the lower-triangle
# CSC a joint fit keeps per cell, with the cells' modes and weights.
make_Q <- function(tau) {
Q <- matrix(0, 12, 12)
Q[1:2, 1:2] <- diag(2, 2) + 0.1
Q[3:12, 3:12] <- tau * crossprod(diff(diag(10))) + diag(0.3, 10)
Q[1, 3:12] <- Q[3:12, 1] <- 0.1
L <- Matrix::tril(methods::as(methods::as(Q, "generalMatrix"),
"CsparseMatrix"))
list(p = L@p, i = L@i, x = L@x)
}
cells <- list(make_Q(1), make_Q(4))
set.seed(1)
modes <- matrix(rnorm(2 * 12, sd = 0.2), 2, 12)
mix <- tulpa_joint_inner_vcov_mixture(
lapply(cells, `[[`, "p"), lapply(cells, `[[`, "i"), lapply(cells, `[[`, "x"),
n_x = 12L, idx = 1:12, n_dense = 2L, A_cols_list = list(3:12),
weights = c(0.7, 0.3), modes = modes)
mix$mean[1:2]
mix$vcov[1:2, 1:2]