Covariance structures with glmmTMB

Overview

This vignette demonstrates some of the covariance structures available in the glmmTMB package. The currently available covariance structures are:

Covariance	Notation	no. parameters	Requirement	Parameters
Unstructured (general positive definite)	`us`	$n(n+1)/2$		See Mappings
Heterogeneous Toeplitz	`toep`	$2n-1$		log-standard deviations ($\theta_1-\theta_n$); correlations $\rho_k = \theta_{n+k}/\sqrt{1+\theta_{n+k}^2}$, $k = \textrm{abs}(i-j+1)$
Het. compound symmetry	`cs`	$n+1$		log-SDs ($\theta_1-\theta_n$); correlation $\{a=1/(n-1); \rho = \textrm{plogis}(\theta_{n+1}) \cdot (1+a) -a \}$
Homogeneous compound symmetry	`homcs`	$2$		log-SD ($\theta_1$); correlation $\{a=1/(n-1); \rho = \textrm{plogis}(\theta_{2}) \cdot (1+a) -a \}$
Homogenous diagonal	`homdiag`	$1$		log-SD
Het. diagonal	`diag`	$n$		log-SDs
AR(1)	`ar1`	$2$	Unit spaced levels	log-SD; $\rho = \left(\theta_2/\sqrt{1+\theta_2^2}\right)^{d_{ij}}$
Het. AR(1)	`hetar1`	$n + 1$	Unit spaced levels	log-SDs ($\theta_1-\theta_n$); $\rho = \left(\theta_2/\sqrt{1+\theta_2^2}\right)^{d_{ij}}$
Ornstein-Uhlenbeck	`ou`	$2$	Coordinates	log-SD; log-OU rate ($\rho = \exp(-\exp(\theta_2) d_{ij})$)
Spatial exponential	`exp`	$2$	Coordinates	log-SD; log-scale ($\rho = \exp(-\exp(-\theta_2) d_{ij})$)
Spatial Gaussian	`gau`	$2$	Coordinates	log-SD; log-scale ($\rho = \exp(-\exp(-2\theta_2) d_{ij}^2$)
Spatial Matèrn	`mat`	$3$	Coordinates	log-SD, log-range, log-shape (power)
Reduced-rank	`rr`	$nd-d(d-1)/2$	rank (d)	Factor loading matrix (see Reduced-rank)
Proportional	`propto`	$1$	Variance-covariance matrix	log(proportionality constant)

The word 'heterogeneous' refers to the marginal variances of the model; $\textrm{plogis}(x) = (1+\exp(-x))^{-1}$

Homogenous versions of some structures (e.g. Toeplitz, compound symmetric) can be implemented by using the map argument to set all log-SD parameters equal to each other.

Some of the structures require temporal or spatial coordinates. We will show examples in a later section.

The AR(1) covariance structure

Demonstration on simulated data

First, let's consider a simple time series model. Assume that our measurements $Y(t)$ are given at discrete times $t \in \{1,...,n\}$ by

\[Y(t) = \mu + X(t) + \varepsilon(t)\]

where

$\mu$ is the mean value parameter.
$X(t)$ is a stationary AR(1) process, i.e. has covariance $cov(X(s), X(t)) = \sigma^2\exp(-\theta |t-s|)$.
$\varepsilon(t)$ is iid. $N(0,\sigma_0^2)$ measurement error.

A simulation experiment is set up using the parameters

Description	Parameter	Value
Mean	$\mu$	0
Process variance	$\sigma^2$	1
Measurement variance	$\sigma_0^2$	1
One-step correlation	$\phi$	0.7

The following R-code draws a simulation based on these parameter values. For illustration purposes we consider a very short time series.

n <- 25                                              ## Number of time points
x <- MASS::mvrnorm(mu = rep(0,n),
             Sigma = .7 ^ as.matrix(dist(1:n)) )    ## Simulate the process using the MASS package
y <- x + rnorm(n)                                   ## Add measurement noise

In order to fit the model with glmmTMB we must first specify a time variable as a factor. The factor levels correspond to unit spaced time points. It is a common mistake to forget some factor levels due to missing data or to order the levels incorrectly. We therefore recommend to construct factors with explicit levels, using the levels argument to the factor function:

times <- factor(1:n, levels=1:n)
head(levels(times))

We also need a grouping variable. In the current case there is only one time-series so the grouping is:

group <- factor(rep(1,n))

We combine the data into a single data frame (not absolutely required, but good practice):

dat0 <- data.frame(y, times, group)

Now fit the model using

glmmTMB(y ~ ar1(times + 0 | group), data=dat0)

This formula notation follows that of the lme4 package.

The left hand side of the bar times + 0 corresponds to a design matrix $Z$ linking observation vector $y$ (rows) with a random effects vector $u$ (columns) (see Construction of structured covariance matrices for why we need the + 0)
The distribution of $u$ is ar1 (this is the only glmmTMB specific part of the formula).
The right hand side of the bar splits the above specification independently among groups. Each group has its own separate $u$ vector but shares the same parameters for the covariance structure.

After running the model, we find the parameter estimates $\mu$ (intercept), $\sigma_0^2$ (dispersion), $\sigma$ (Std. Dev.) and $\phi$ (First off-diagonal of "Corr") in the output:

For those trying to make sense of the internal parameterization, the internal transformation from the parameter ($\theta_2$) to the AR1 coefficient ($\phi$) is $\phi = \theta_2/\sqrt(1+\theta_2^2)$; the inverse transformation is $\theta_2 = \phi/\sqrt(1-\phi^2)$. (The first element of the theta vector is the log-standard-deviation.)

Increasing the sample size

A single time series of 6 time points is not sufficient to identify the parameters. We could either increase the length of the time series or increase the number of groups. We'll try the latter:

simGroup <- function(g, n=6, phi=0.7) {
    x <- MASS::mvrnorm(mu = rep(0,n),
             Sigma = phi ^ as.matrix(dist(1:n)) )   ## Simulate the process
    y <- x + rnorm(n)                               ## Add measurement noise
    times <- factor(1:n)
    group <- factor(rep(g,n))
    data.frame(y, times, group)
}
simGroup(1)

Generate a dataset with 1000 groups:

dat1 <- do.call("rbind", lapply(1:1000, simGroup) )

And fitting the model on this larger dataset gives estimates close to the true values (AR standard deviation=1, residual (measurement) standard deviation=1, autocorrelation=0.7):

(fit.ar1 <- glmmTMB(y ~ ar1(times + 0 | group), data=dat1))

The unstructured covariance

We can try to fit an unstructured covariance to the previous dataset dat. For this case an unstructured covariance has 300 correlation parameters and 25 variance parameters. Adding $\sigma_0^2 I$ on top would cause a strict overparameterization, as these would be redundant with the diagonal elements in the covariance matrix. Hence, when fitting the model with glmmTMB, we have to disable the $\varepsilon$ term (the dispersion) by setting dispformula=~0:

fit.us <- glmmTMB(y ~ us(times + 0 | group), data=dat1, dispformula=~0)
fit.us$sdr$pdHess ## Converged ?

The estimated variance and correlation parameters are:

VarCorr(fit.us)

The estimated correlation is approximately constant along diagonals (apparent Toeplitz structure) and we note that the first off-diagonal is now ca. half the true value (0.7) because the dispersion is effectively included in the estimated covariance matrix (i.e. $\rho' = \rho {\sigma^2_{{\text {AR}}}}/({\sigma^2_{{\text {AR}}}} + {\sigma^2_{{\text {meas}}}})$).

The Toeplitz structure

The next natural step would be to reduce the number of parameters by collecting correlation parameters within the same off-diagonal. This amounts to 24 correlation parameters and 25 variance parameters.

We use dispformula = ~0 to suppress the residual variance (it actually gets set to a small value controlled by the zerodisp_val argument of glmmTMBControl())¹

fit.toep <- glmmTMB(y ~ toep(times + 0 | group), data=dat1,
                    dispformula=~0)
fit.toep$sdr$pdHess ## Converged ?

The estimated variance and correlation parameters are:

(vc.toep <- VarCorr(fit.toep))

The diagonal elements are all approximately equal to the true total variance (${\sigma^2_{{\text {AR}}}} + {\sigma^2_{{\text {meas}}}}$=2), and the off-diagonal elements are approximately equal to the expected value of 0.7/2=0.35.

vc1 <- vc.toep$cond[[1]] ## first term of var-cov for RE of conditional model
summary(diag(vc1))
summary(vc1[row(vc1)!=col(vc1)])

We can get a slightly better estimate of the variance by using REML estimation (however, the estimate of the correlations seems to have gotten slightly worse):

fit.toep.reml <- update(fit.toep, REML=TRUE)
vc1R <- VarCorr(fit.toep.reml)$cond[[1]]
summary(diag(vc1R))
summary(vc1R[row(vc1R)!=col(vc1R)])

Compound symmetry

The compound symmetry structure collects all off-diagonal elements of the correlation matrix to one common value.

We again use dispformula = ~0 to make the model parameters identifiable (see the footnote in The Toeplitz structure; a similar, although slightly simpler, argument applies here).

fit.cs <- glmmTMB(y ~ cs(times + 0 | group), data=dat1, dispformula=~0)
fit.cs$sdr$pdHess ## Converged ?

The estimated variance and correlation parameters are:

VarCorr(fit.cs)

Anova tables

The models ar1, toep, and us are nested so we can use:

anova(fit.ar1, fit.toep, fit.us)

ar1 has the lowest AIC (it's the simplest model, and fits the data adequately); we can't reject the (true in this case!) null model that an AR1 structure is adequate to describe the data.

The model cs is a sub-model of toep:

anova(fit.cs, fit.toep)

Here we can reject the null hypothesis of compound symmetry (i.e., that all the pairwise correlations are the same).

Adding coordinate information

Coordinate information can be added to a variable using the glmmTMB function numFactor. This is necessary in order to use those covariance structures that require coordinates. For example, if we have the numeric coordinates

x <- sample(1:2, 10, replace=TRUE)
y <- sample(1:2, 10, replace=TRUE)

we can generate a factor representing $(x,y)$ coordinates by

(pos <- numFactor(x,y))

Numeric coordinates can be recovered from the factor levels:

parseNumLevels(levels(pos))

In order to try the remaining structures on our test data we re-interpret the time factor using numFactor:

dat1$times <- numFactor(dat1$times)
levels(dat1$times)

Ornstein–Uhlenbeck

Having the numeric times encoded in the factor levels we can now try the Ornstein–Uhlenbeck covariance structure.

fit.ou <- glmmTMB(y ~ ou(times + 0 | group), data=dat1)
fit.ou$sdr$pdHess ## Converged ?

It should give the exact same results as ar1 in this case since the times are equidistant:

VarCorr(fit.ou)

However, note the differences between ou and ar1:

ou can handle irregular time points.
ou only allows positive correlation between neighboring time points.

Spatial correlations

The structures exp, gau and mat are meant to used for spatial data. They all require a Euclidean distance matrix which is calculated internally based on the coordinates. Here, we will try these models on the simulated time series data.

An example with spatial data is presented in a later section.

Matern

fit.mat <- glmmTMB(y ~ mat(times + 0 | group), data=dat1, dispformula=~0)
fit.mat$sdr$pdHess ## Converged ?

VarCorr(fit.mat)

Gaussian

"Gaussian" refers here to a Gaussian decay in correlation with distance, i.e. $\rho = \exp(-d x^2)$, not to the conditional distribution ("family").

fit.gau <- glmmTMB(y ~ gau(times + 0 | group), data=dat1, dispformula=~0)
fit.gau$sdr$pdHess ## Converged ?

VarCorr(fit.gau)

Exponential

fit.exp <- glmmTMB(y ~ exp(times + 0 | group), data=dat1)
fit.exp$sdr$pdHess ## Converged ?

VarCorr(fit.exp)

A spatial covariance example

Starting out with the built in volcano dataset we reshape it to a data.frame with pixel intensity z and pixel position x and y:

d <- data.frame(z = as.vector(volcano),
                x = as.vector(row(volcano)),
                y = as.vector(col(volcano)))

Next, add random normal noise to the pixel intensities and extract a small subset of 100 pixels. This is our spatial dataset:

set.seed(1)
d$z <- d$z + rnorm(length(volcano), sd=15)
d <- d[sample(nrow(d), 100), ]

Display sampled noisy volcano data:

volcano.data <- array(NA, dim(volcano))
volcano.data[cbind(d$x, d$y)] <- d$z
image(volcano.data, main="Spatial data", useRaster=TRUE)

Based on this data, we'll attempt to re-construct the original image.

As model, it is assumed that the original image image(volcano) is a realization of a random field with correlation decaying exponentially with distance between pixels.

Denoting by $u(x,y)$ this random field the model for the observations is

\[ z_{i} = \mu + u(x_i,y_i) + \varepsilon_i \]

To fit the model, a numFactor and a dummy grouping variable must be added to the dataset:

d$pos <- numFactor(d$x, d$y)
d$group <- factor(rep(1, nrow(d)))

The model is fit by

f <- glmmTMB(z ~ 1 + exp(pos + 0 | group), data=d)

Recall that a standard deviation sd=15 was used to distort the image. A confidence interval for this parameter is

confint(f, "sigma")

The glmmTMB predict method can predict unseen levels of the random effects. For instance to predict a 3-by-3 corner of the image one could construct the new data:

newdata <- data.frame( pos=numFactor(expand.grid(x=1:3,y=1:3)) )
newdata$group <- factor(rep(1, nrow(newdata)))
newdata

and predict using

predict(f, newdata, type="response", allow.new.levels=TRUE)

A specific image column can thus be predicted using the function

predict_col <- function(i) {
    newdata <- data.frame( pos = numFactor(expand.grid(1:87,i)))
    newdata$group <- factor(rep(1,nrow(newdata)))
    predict(f, newdata=newdata, type="response", allow.new.levels=TRUE)
}

Prediction of the entire image is carried out by (this takes a while...):

pred <- sapply(1:61, predict_col)

Finally plot the re-constructed image by

image(pred, main="Reconstruction")

Mappings

For various advanced purposes, such as computing likelihood profiles, it is useful to know the details of the parameterization of the models - the scale on which the parameters are defined (e.g. standard deviation, variance, or log-standard deviation for variance parameters) and their order.

Unstructured

For an unstructured matrix of size n, parameters 1:n represent the log-standard deviations while the remaining n(n-1)/2 (i.e. (n+1):(n:(n*(n+1)/2))) are the elements of the scaled Cholesky factor of the correlation matrix, filled in row-wise order (see TMB documentation). In particular, if $L$ is the lower-triangular matrix with 1 on the diagonal and the correlation parameters in the lower triangle, then the correlation matrix is defined as $\Sigma = D^{-1/2} L L^\top D^{-1/2}$, where $D = \textrm{diag}(L L^\top)$. For a single correlation parameter $\theta_0$, this works out to $\rho = \theta_0/\sqrt{1+\theta_0^2}$ (with inverse $\theta_0 = \rho/\sqrt(1-\rho^2)$. You can use the utility functions get_cor() (transform a theta vector into the upper triangular [rowwise] elements of a correlation matrix, or the full correlation matrix) and put_cor() (translate a correlation matrix, or the values from the lower triangle, into a theta vector) to perform these transformations.

(See calculations here.)

vv0 <- VarCorr(fit.us)
vv1 <- vv0$cond$group          ## extract 'naked' V-C matrix
n <- nrow(vv1)
rpars <- getME(fit.us,"theta") ## extract V-C parameters
## first n parameters are log-std devs:
all.equal(unname(diag(vv1)),exp(rpars[1:n])^2)
## now try correlation parameters:
cpars <- rpars[-(1:n)]
length(cpars)==n*(n-1)/2      ## the expected number
cc <- diag(n)
cc[upper.tri(cc)] <- cpars
L <- crossprod(cc)
D <- diag(1/sqrt(diag(L)))
round(D %*% L %*% D,3)
round(unname(attr(vv1,"correlation")),3)

all.equal(c(cov2cor(vv1)),c(fit.us$obj$env$report(fit.us$fit$parfull)$corr[[1]]))

Profiling (experimental/exploratory):

## want $par, not $parfull: do NOT include conditional modes/'b' parameters
ppar <- fit.us$fit$par
length(ppar)
range(which(names(ppar)=="theta")) ## the last n*(n+1)/2 parameters
## only 1 fixed effect parameter
tt <- tmbprofile(fit.us$obj,2,trace=FALSE)

confint(tt)
plot(tt)

ppar <- fit.cs$fit$par
length(ppar)
range(which(names(ppar)=="theta")) ## the last n*(n+1)/2 parameters
## only 1 fixed effect parameter, 1 dispersion parameter
tt2 <- tmbprofile(fit.cs$obj,3,trace=FALSE)

plot(tt2)

Generalized latent variable model

Consider a generalized linear mixed model

\[\begin{equation} g(\boldsymbol{\mu}) = \boldsymbol{X\beta} + \boldsymbol{Zb} \end{equation}\]

where $g(.)$ is the link function; $\boldsymbol{\beta}$ is a p-dimensional vector of regression coefficients related to the covariates; $\boldsymbol{X}$ is an $n \times p$ model matrix; and $\boldsymbol{Z}$ is the $n\times q$ model matrix for the $q$-dimensional vector-valued random effects variable $\boldsymbol{U}$ which is multivariate normal with mean zero and a parameterized $q \times q$ variance-covariance matrix, $\boldsymbol{\Sigma}$, i.e., $\boldsymbol{U} \sim N(\boldsymbol{0}, \boldsymbol{\Sigma})$.

A general latent variable model (GLVM) requires many fewer parameters for the variance-covariance matrix, $\boldsymbol{\Sigma}$. To a fit a GLVM we add a reduced-rank (rr) covariance structure, so the model becomes \[\begin{align} g(\boldsymbol{\mu}) &= \boldsymbol{X\beta} + \boldsymbol{Z(I_n \otimes \Lambda)b} \\ &= \boldsymbol{X\beta} + \boldsymbol{Zb_{new}} \end{align}\]

where $\otimes$ is the Kronecker product and $\boldsymbol{\Lambda} = (\boldsymbol{\lambda_1}, \ldots, \boldsymbol{\lambda_d})'$ is the $q \times d$ matrix of factor loadings (with $d \ll q$). The upper triangular elements of $\boldsymbol{\Lambda}$ are set to be zero to ensure parameter identifiability. Here we assume that the latent variables follow a multivariate standard normal distribution, $\boldsymbol{b} \sim N(\boldsymbol{0}, \boldsymbol{I})$.

For GLVMs it is important to select initial starting values for the parameters because the observed likelihood may be multimodal, and maximization algorithms can end up in local maxima. Niku et al. (2019) describe methods to enable faster and more reliable fits of latent variable models by carefully choosing starting values of the parameters.

A similar method has been implemented in glmmTMB (McGillycuddy et al., n.d.). A generalized linear model is fitted to the data to obtain initial starting values for the fixed parameters in the model. Residuals from the fitted GLM are calculated; Dunn-Smyth residuals are calculated for common families while residuals from the dev.resids() function are used otherwise. Initial starting values for the latent variables and their loadings are obtained by fitting a reduced rank model to the residuals.

Reduced-rank

One of our main motivations for adding this variance-covariance structure is to enable the analysis of multivariate abundance data, for example to model the abundance of different taxa across multiple sites. Typically an unstructured random effect is assumed to account for correlation between taxa; however the number of parameters required quickly becomes large with increasing numbers of taxa. A GLVM is a flexible and more parsimonious way to account for correlation so that one can fit a joint model across many taxa.

A GLVM can be fit by specifying a reduced rank (rr) covariance structure. For example, the code for modeling the mean abundance against taxa and to account for the correlation between taxa using two latent variables is as follows

## fit rank-reduced models with varying dimension
dvec <- 2:10
fit_list <- lapply(dvec,
                   function(d) {
                       glmmTMB(abund ~ Species + rr(Species + 0|id, d = d),
                               data = spider_long)
                   })
names(fit_list) <- dvec
## compare fits via AIC
aic_vec <- sapply(fit_list, AIC)
delta_aic  <- aic_vec - min(aic_vec, na.rm = TRUE)

The left hand side of the bar taxa + 0 corresponds to a factor loading matrix that accounts for the correlations among taxa. The right hand side of the bar splits the above specification independently among sites. The d is a non-negative integer (which defaults to 2).

An option in glmmTMBControl() has been included to initialize the starting values for the parameters based on the approach mentioned above with the default set at glmmTMBControl(start_method = list(method = NULL, jitter.sd = 0):

method = "res" initializes starting values from the results of fitting a GLM, and fitting a reduced rank model to the residuals to obtain starting values for the fixed coefficients, the latent variables and the factor loadings.
jitter.sd adds variation to the starting values of latent variables when method = "res" (default 0).

For a reduced rank matrix of rank d, parameters 1:d represent the diagonal factor loadings while the remaining $nd-d(d-3)/2$, (i.e. parameters (d+1):(nd-d(d-1)/2) are the lower diagonal factor loadings filled in column-wise order. The factor loadings from a model can be obtained by fit.rr$obj$env$report(fit.rr$fit$parfull)$fact_load[[1]]. An appropriate rank for the model can be determined by standard model selection approaches such as information criteria (e.g. AIC or BIC) (F. K. Hui et al. 2015).

We can extract the random effects (predicted values for each site by species combination) with ranef(); `as.data.frame(ranef()) (or broom.mixed::tidy(..., effects = "ran_vals")) gives the results in a more convenient format. Based on this information, we can plot the predictions for species (ordered by their predicted presence at site 1). (We've arbitrarily chosen d=3 here.)

spider_rr <- glmmTMB(abund ~ Species + rr(Species + 0|id, d = 3),
                     data = spider_long)
re <- as.data.frame(ranef(spider_rr))
re <- within(re, {
    ## sites in numeric order
    grp <- factor(grp, levels = unique(grp))
    ## species in site-1-predicted-abundance order
    term <- reorder(term, condval, function(x) x[1])
    lwr <- condval - 2*condsd
    upr <- condval + 2*condsd
})
if (require("ggplot2")) {
    ggplot(re, aes(grp, condval)) +
        geom_pointrange(aes(ymin=lwr, ymax = upr)) +
        facet_wrap(~term, scale = "free")
}

If we instead want to get the factor loadings by Species and latent variables by site, we can use a (so far experimental) function to get a list with components $fl (factor loadings) and $b (latent variables by site)

source(system.file("misc", "extract_rr.R", package = "glmmTMB"))
rr_info <- extract_rr(spider_rr)
lapply(rr_info, dim)

We can use this information to create an (ugly) biplot. (Improvements welcome!)

par(las = 1)
afac <- 4
sp_names <- abbreviate(gsub("Species", "", rownames(rr_info$fl)))
plot(rr_info$fl[,1], rr_info$fl[,2], xlab = "factor 1", ylab = "factor 2", pch = 16, cex = 2)
text(rr_info$b[,1]*afac*1.05, rr_info$b[,2]*afac*1.05, rownames(rr_info$b))
arrows(0, 0, rr_info$b[,1]*afac, rr_info$b[,2]*afac)
text(rr_info$fl[,1], rr_info$fl[,2], sp_names, pos = 3, col = 2)

Proportional

The random effect structure propto fits multivariate random effects proportional to a known variance-covariance matrix. One way the propto structure can be used is in phylogenetic analysis where a random effect proportional to a phylogenetic variance-covariance matrix aims to account for the correlation across species due to their shared ancestry. For example, the carni70 data set from the ade4 package describes the phylogeny along with the geographic range and body size of 70 carnivora. To account for the dependence among species due to shared ancestral history we can include a phylogenetically structured error term in the model via the propto structure as follows:

library(ape)
data(carni70, package = "ade4")
tree <- read.tree(text = carni70$tre)
phylo_varcov <- vcv(tree)# phylogenetic variance-covariance matrix
## row/column names of phylo_varcov must match factor levels in data
## (punctuation/separators in species names and ordering)
spnames <- gsub("_", ".", rownames(carni70$tab))
carnidat <- data.frame(
    species = factor(spnames, levels = rownames(phylo_varcov)),
    dummy = factor(1),
    carni70$tab)
fit_phylo <- glmmTMB(log(range) ~ log(size) +
                         propto(0 + species | dummy, phylo_varcov),
                     data = carnidat)

dummy is a dummy variable equal to one for all observations to specify that all observations belong to the same cluster. The intercept term is excluded from the proportional random effect -- this is to ensure that each random effect corresponds to the effect for its corresponding species. It is important that the row/column names of the matrix match the terms in the random effect (i.e. the same values, in the same order). In particular, this typically means that the levels of the varying factor (species, in the case of a phylogenetic model) should match the row/column names of the covariance matrix. Something like data$species <- factor(data$species, levels = rownames(covmat)) should generally work. See Construction of structured covariance matrices for how the terms are constructed).

Construction of structured covariance matrices

This section will explain how covariance matrices are constructed "under the hood", and in particular why the 0+ term is generally required in models for temporal and spatial covariances.

Probably the key insight here is that the terms in a random effect (the f formula in a random-effects term (f|g) are expanded using the base-R machinery for regression model formulas. In the case of an intercept-only random effect (1|g), the model matrix is a column of ones, so we have a $1 \times 1$ covariance matrix - a single variance. For a random-slopes model (x|g) or (1+x|g), where x is a numeric variable, the model matrix has two columns, a column of ones and column of observed values of x, and the covariance matrix is $2 \times 2$ (intercept variance, slope variance, intercept-slope covariance).

Things start to get weird when we have (f|g) (or (1+f|g)) where f is a factor (representing a categorical variable). R uses treatment contrasts by default; if the observed values of f are c("c", "s", "v")² the corresponding factor will have a baseline level of "c" by default, and the model matrix will be:

model.matrix(~f, data.frame(f=factor(c("c", "s", "v"))))

##   (Intercept) fs fv
## 1           1  0  0
## 2           1  1  0
## 3           1  0  1
## attr(,"assign")
## [1] 0 1 1
## attr(,"contrasts")
## attr(,"contrasts")$f
## [1] "contr.treatment"

i.e., an intercept (which corresponds to the predicted mean value for observations in group c) followed by dummy variables that describe contrasts between the predicted mean values for s and c (fs) and between v and c (fv). The covariance matrix is $3 \times 3$ and looks like this:

\[ \newcommand{\ssub}[1]{\sigma^2_{\textrm{#1}}} \newcommand{\csub}[2]{\sigma^2_{\textrm{#1}, \textrm{#2}}} \left( \begin{array}{ccc} \ssub{c} & \csub{c}{s-c} & \csub{c}{v-c} \\ \csub{c}{s-c} & \ssub{s-c} & \csub{s-c}{v-c} \\ \csub{c}{v-c} & \csub{s-c}{v-c} & \ssub{v-c} \end{array} \right) \]

This might be OK for some problems, but the parameters of the model will often be more interpretable if we remove the intercept from the formula:

model.matrix(~0+f, data.frame(f=factor(c("c", "s", "v"))))

##   fc fs fv
## 1  1  0  0
## 2  0  1  0
## 3  0  0  1
## attr(,"assign")
## [1] 1 1 1
## attr(,"contrasts")
## attr(,"contrasts")$f
## [1] "contr.treatment"

The corresponding covariance matrix is

\[ \left( \begin{array}{ccc} \ssub{c} & \csub{c}{s} & \csub{c}{v} \\ \csub{c}{s} & \ssub{s} & \csub{s}{v} \\ \csub{c}{v} & \csub{s}{v} & \ssub{v} \end{array} \right) \]

This is easier to understand (the elements are the variances of the intercepts for each group, and the covariances between intercepts of different groups). If we use an 'unstructured' model (us(f|g), or just plain (f|g)), then this reparameterization won't make any difference in the overall model fit. However, if we use a structured covariance model, then the choice matters: for example, the two models diag(f|g) and diag(0+f|g) give rise to the covariance matrices

\[ \left( \begin{array}{ccc} \ssub{c} & 0 & 0 \\ 0 & \ssub{s-c} & 0 \\ 0 & 0 & \ssub{v-c} \end{array} \right) \;\; \textrm{vs} \;\; \left( \begin{array}{ccc} \ssub{c} & 0 & 0 \\ 0 & \ssub{s} & 0 \\ 0 & 0 & \ssub{v} \end{array} \right) \]

which cannot be made equivalent by changing parameters.

What does this have to do with temporally/spatially structured covariance matrices? In this case, if two points are separated by a distance $d_{ij}$ (in space or time), we typically want their correlation to be $\sigma^2 \rho(d_{ij})$, where $\rho()$ is a temporal or spatial autocorrelation function (e.g. in the AR1 model, $\rho(d_{ij}) = \phi^{d_{ij}}$). So we want to set up a covariance matrix

\[ \sigma^2 \left( \begin{array}{cccc} 1 & \rho(d_{12}) & \rho(d_{13}) & \ldots \\ \rho(d_{12}) & 1 & \rho(d_{23}) & \ldots \\ \rho(d_{13}) & \rho(d_{23}) & 1 & \ldots \\ \vdots & \vdots & \vdots & \ddots \end{array} \right) \]

How glmmTMB actually does this internally is to

treat the temporal/spatial locations as a factor to construct the data structure for a $n \times n$ covariance matrix (where $n$ is the number of unique locations)
use the information encoded in the levels by numFactor() to compute the corresponding pairwise distances
use the prefix of the random term (e.g. ar1 or ou) and the autocorrelation parameters (drawn from the parameter vector) to specify the autocorrelation function
use the autocorrelation function and the distances to fill in the values in the correlation matrix
multiply the correlation matrix by the variance (also drawn from the parameter vector) to compute the covariance matrix

In order for this to work, we need the $i^\textrm{th}$ column of the corresponding model matrix to correspond to an indicator variable for whether an observation is at the $i^\textrm{th}$ location --- not to a contrast between the $i\textrm{th}$ level and the first level! So, we want to use e.g. ar1(0 + time|g), not ar1(time|g) (which is equivalent to ar1(1+time|g)).

Why do we do this? Consider the slightly simplified case of a homogeneous Toeplitz structure where all of the variance parameters are identical. The diagonal elements of the covariance matrix are equal to $\sigma_t^2$, the off-diagonals to $\sigma_t^2 \cdot \rho(|i-j|)$. If we add a residual variance to the model then the diagonal of the combined covariance matrix becomes $\sigma_t^2 + \sigma_r^2$ and the off-diagonals become $(\sigma_t^2 + \sigma_r^2) \rho(|i-j|)$. However, by reparameterizing the Toeplitz model to $\{{\sigma_t^2}' = \sigma_t^2 + \sigma_r^2, \rho'(|i-j|) = \rho(|i-j|) \cdot \frac{\sigma_t^2}{\sigma_t^2 + \sigma_r^2}\}$ --- that is, by inflating the variance and deflating the correlation parameters --- we can get back to an equivalent Toeplitz model. This implies that the residual variance and the Toeplitz covariance parameters are jointly unidentifiable, which is likely to make problems for the fitting procedure.↩
chocolate, strawberry, vanilla↩

Covariance structures with glmmTMB

Kasper Kristensen and Maeve McGillycuddy

2025-08-16

Overview

The AR(1) covariance structure

Demonstration on simulated data

Increasing the sample size

The unstructured covariance

The Toeplitz structure

Compound symmetry

Anova tables

Adding coordinate information

Ornstein–Uhlenbeck

Spatial correlations

Matern

Gaussian

Exponential

A spatial covariance example

Mappings

Unstructured

Generalized latent variable model

Reduced-rank

Proportional

Construction of structured covariance matrices

References

Covariance	Notation	no. parameters	Requirement	Parameters
Unstructured (general positive definite)	`us`	\(n(n+1)/2\)		See Mappings
Heterogeneous Toeplitz	`toep`	\(2n-1\)		log-standard deviations (\(\theta_1-\theta_n\)); correlations \(\rho_k = \theta_{n+k}/\sqrt{1+\theta_{n+k}^2}\), \(k = \textrm{abs}(i-j+1)\)
Het. compound symmetry	`cs`	\(n+1\)		log-SDs (\(\theta_1-\theta_n\)); correlation \(\{a=1/(n-1); \rho = \textrm{plogis}(\theta_{n+1}) \cdot (1+a) -a \}\)
Homogeneous compound symmetry	`homcs`	\(2\)		log-SD (\(\theta_1\)); correlation \(\{a=1/(n-1); \rho = \textrm{plogis}(\theta_{2}) \cdot (1+a) -a \}\)
Homogenous diagonal	`homdiag`	\(1\)		log-SD
Het. diagonal	`diag`	\(n\)		log-SDs
AR(1)	`ar1`	\(2\)	Unit spaced levels	log-SD; \(\rho = \left(\theta_2/\sqrt{1+\theta_2^2}\right)^{d_{ij}}\)
Het. AR(1)	`hetar1`	\(n + 1\)	Unit spaced levels	log-SDs (\(\theta_1-\theta_n\)); \(\rho = \left(\theta_2/\sqrt{1+\theta_2^2}\right)^{d_{ij}}\)
Ornstein-Uhlenbeck	`ou`	\(2\)	Coordinates	log-SD; log-OU rate (\(\rho = \exp(-\exp(\theta_2) d_{ij})\))
Spatial exponential	`exp`	\(2\)	Coordinates	log-SD; log-scale (\(\rho = \exp(-\exp(-\theta_2) d_{ij})\))
Spatial Gaussian	`gau`	\(2\)	Coordinates	log-SD; log-scale (\(\rho = \exp(-\exp(-2\theta_2) d_{ij}^2\))
Spatial Matèrn	`mat`	\(3\)	Coordinates	log-SD, log-range, log-shape (power)
Reduced-rank	`rr`	\(nd-d(d-1)/2\)	rank (d)	Factor loading matrix (see Reduced-rank)
Proportional	`propto`	\(1\)	Variance-covariance matrix	log(proportionality constant)

Description	Parameter	Value
Mean	\(\mu\)	0
Process variance	\(\sigma^2\)	1
Measurement variance	\(\sigma_0^2\)	1
One-step correlation	\(\phi\)	0.7