Exponential Family
\[
f(y_i\vert \theta_i,\phi)=\exp\left\{ \frac{y_i\theta_i-
b(\theta_i)}{a(\phi)}+c(y_i,\phi)\right\}
\]
likelihood to observe \(y_1, \ldots,
y_n\) independent observations \[L(\boldsymbol{\theta},\phi\vert
\boldsymbol{y})=\prod\limits_{i=1}^n f(y_i,\theta_i,\phi)\]
log-likelihood \[
l(\boldsymbol{\theta},\phi\vert \boldsymbol{y}) = \sum\limits_{i=1}^n
\log f(y_i,\theta_i,\phi)
\]
Log-likelihood for one observation: \[
l(\theta_i,\phi\vert y_i)=\left\{ \frac{y_i\theta_i-
b(\theta_i)}{a(\phi)}+c(y_i,\phi)\right\}
\]
- \(E[y_i]=\mu_i=b^\prime(\theta_i)\)
- \(\text{var}[y_i]=b^{\prime\prime}(\theta_i) a(\phi)
=V(\mu_i)\)
e.g. for Poisson data: \(\text{var}[y_i] =
\mu_i\) and for negative binomial data \(\text{var}[y_i] = \mu_i + \phi
\mu_i^2\).
Parameter Estimation:
Maximum Likelihood
\[
S(\boldsymbol{\beta}) = \frac{\partial l(\boldsymbol{\mu} \vert
\mathbf{y})}{
\partial{\boldsymbol{\beta}}} = 0
\]
\[
S_i(\boldsymbol{\beta})=
\frac{y_i-\mu_i}{\text{var}[y_i]}\frac{\partial\mu}{\partial\eta}\mathbf{x}_i
\]
There are only two moments involved in the estimation equations of
the mean model parameters: the mean and the variance!
\[
S(\boldsymbol{\beta})=\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right)
= 0
\]
We can solve this set of score equations iteratively to estimate the
model parameters: \[
\mathbf{\beta}^{k+1} =
(\mathbf{X}^T\mathbf{W}^k\mathbf{X})^{-1}\mathbf{X}^T\mathbf{W}^kz^{k}
\]
with pseudodata
\[
z^k_i = \eta^k_i + \left.\frac{\partial \eta_i}{\partial
\mu_i}\right\vert_k (y_i - \mu^k_i)
\]
Quasi-likelihood
We no longer define the full distribution but only two moments: the
mean and the variance of \(y_i\).
We typically define these based on an existing
distribution.
However we make the variance more flexible, i.e. we rescale it
with an additional model parameter.
Hence, we can model data that are over or under disperse with
respect to a known distribution.
\[
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 V(\mu_i)
\end{array}\right.
\]
e.g. quasi poisson
\[
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 \mu_i
\end{array}\right.
\]
e.g. quasi-negative binomial
\[
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 (\mu_i + \phi \mu_i^2)
\end{array}\right.
\]
Parameter
Estimation
Note, that this leads to the following estimation equations:
\[
U_i(\boldsymbol{\beta})=
\frac{y_i-\mu_i}{\sigma^2V(\mu_i)}\frac{\partial\mu}{\partial\eta}\mathbf{x}_i
\]
\[
\begin{array}{rcccc}
U(\boldsymbol{\beta})&=&\left[\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right)\right]/\sigma^2
&=& 0\\
&&\Updownarrow\\
&&\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right)
&=& 0
\end{array}
\] Hence, the estimating equations for the mean model parameters
remain the same as those for the conventional distribution where the
quasi-likelihood is derived from.
The variance covariance matrix of the mean model parameters then
becomes: \[
\Sigma_{\hat{\boldsymbol{\beta}}}=
(\mathbf{X}^T\mathbf{WX})^{-1}\sigma^2
\]
We can estimate \(\sigma^2\) using a
moment estimator on the residual vector \(\mathbf{y}-\boldsymbol{\mu}\), i.e.
\[
\hat{\sigma}^2 = \frac{1}{n-p} \sum_\limits{i=1}^n
\frac{(y_i-\hat\mu_i)^2}{V(\hat\mu_i)}
\]
Note, that \[e_i^p=\frac{(y_i-\hat\mu_i)}{\sqrt{V(\hat\mu_i)}}\]
are also referred to as the Pearson residuals.
Another type of residuals for GLMs are deviance residuals, i.e.
\[e_i^d =
\text{sign}(y_i-\hat\mu_i)\sqrt{2[l(y_i,y_i)-l(y_i,\hat\mu_i)]}
\] So another estimator is
\[\hat{\sigma}^2 =
\frac{\sum_\limits{i=1}^n(e_i^d)^2}{n-p} = \frac{D}{n-p}
\] with D the deviance statistic: the LRT test between the
saturated model (a model that provides a perfect fit) and the current
model:
\[
D = 2 \sum\limits_{i=1}^n [l(y_i,y_i,\phi)- l(y_i,\hat{\mu}_i,\phi)]
\]
So the standard errors on the model parameters under quasi-likelihood
become:
\[
\hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{QL} =
\hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{ML}\times
\hat{\sigma}\]
Hypothesis tests
An approximate t-test statistic can be defined as
\[
t =
\frac{\mathbf{L}^T\hat{\boldsymbol{\beta}}}{\hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{QL}}
\approx t_{n-p}\vert H_0
\]
And an approximate F-test statistic can be defined as:
\[F =
\frac{\frac{\text{LRT}^{ML}}{c}}{\hat\sigma^2} \approx F_{c,n-p} \vert
H_0,\] with c the degrees of freedom of the LRT statistic.
Example
## quasipoisson.
counts <- c(18,17,15,20,10,20,25,13,12)
outcome <- gl(3,1,9)
treatment <- gl(3,3)
d.AD <- data.frame(treatment, outcome, counts)
d.AD
glm.pois <- glm(counts ~ outcome + treatment, family = poisson())
summary(glm.pois)
##
## Call:
## glm(formula = counts ~ outcome + treatment, family = poisson())
##
## Coefficients:
## Estimate Std. Error z value Pr(>|z|)
## (Intercept) 3.045e+00 1.709e-01 17.815 <2e-16 ***
## outcome2 -4.543e-01 2.022e-01 -2.247 0.0246 *
## outcome3 -2.930e-01 1.927e-01 -1.520 0.1285
## treatment2 1.398e-16 2.000e-01 0.000 1.0000
## treatment3 -2.416e-16 2.000e-01 0.000 1.0000
## ---
## Signif. codes: 0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
##
## (Dispersion parameter for poisson family taken to be 1)
##
## Null deviance: 10.5814 on 8 degrees of freedom
## Residual deviance: 5.1291 on 4 degrees of freedom
## AIC: 56.761
##
## Number of Fisher Scoring iterations: 4
glm.qpois <- glm(counts ~ outcome+treatment, family = quasipoisson())
summary(glm.qpois)
##
## Call:
## glm(formula = counts ~ outcome + treatment, family = quasipoisson())
##
## Coefficients:
## Estimate Std. Error t value Pr(>|t|)
## (Intercept) 3.045e+00 1.944e-01 15.665 9.7e-05 ***
## outcome2 -4.543e-01 2.299e-01 -1.976 0.119
## outcome3 -2.930e-01 2.192e-01 -1.337 0.252
## treatment2 1.398e-16 2.274e-01 0.000 1.000
## treatment3 -2.416e-16 2.274e-01 0.000 1.000
## ---
## Signif. codes: 0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
##
## (Dispersion parameter for quasipoisson family taken to be 1.2933)
##
## Null deviance: 10.5814 on 8 degrees of freedom
## Residual deviance: 5.1291 on 4 degrees of freedom
## AIC: NA
##
## Number of Fisher Scoring iterations: 4
Estimate dispersion ourselves? We first calculate the Pearson
residuals.
ep <- (counts - glm.pois$fitted)/sqrt(glm.pois$fitted)
range(ep - resid(glm.pois,type="pearson"))
## [1] 0 0
Now, we can estimate the quasi-dispersion parameter
n <- length(counts)
p <- length(coef(glm.pois))
sigma2 <- sum(ep^2)/(n-p)
sigma2
## [1] 1.2933
poisRes <- summary(glm.pois)$coef
poisRes
## Estimate Std. Error z value Pr(>|z|)
## (Intercept) 3.044522e+00 0.1708987 1.781478e+01 5.426767e-71
## outcome2 -4.542553e-01 0.2021708 -2.246889e+00 2.464711e-02
## outcome3 -2.929871e-01 0.1927423 -1.520097e+00 1.284865e-01
## treatment2 1.397701e-16 0.2000000 6.988506e-16 1.000000e+00
## treatment3 -2.415657e-16 0.2000000 -1.207829e-15 1.000000e+00
qlRes <- summary(glm.qpois)$coef
qlRes
## Estimate Std. Error t value Pr(>|t|)
## (Intercept) 3.044522e+00 0.1943517 1.566502e+01 9.698855e-05
## outcome2 -4.542553e-01 0.2299154 -1.975750e+00 1.193809e-01
## outcome3 -2.929871e-01 0.2191931 -1.336662e+00 2.522944e-01
## treatment2 1.397701e-16 0.2274467 6.145180e-16 1.000000e+00
## treatment3 -2.415657e-16 0.2274467 -1.062076e-15 1.000000e+00
cbind(ql.se=qlRes[,2],pois.se=poisRes[,2],qlself.se=poisRes[,2]*sqrt(sigma2))
## ql.se pois.se qlself.se
## (Intercept) 0.1943517 0.1708987 0.1943517
## outcome2 0.2299154 0.2021708 0.2299154
## outcome3 0.2191931 0.1927423 0.2191931
## treatment2 0.2274467 0.2000000 0.2274467
## treatment3 0.2274467 0.2000000 0.2274467
Approximate
F-test
LR -test with Poisson regression:
## Warning: package 'car' was built under R version 4.4.1
## Loading required package: carData
We check that the approximate F-statistic equals LRT/df/sigma2
Anova(glm.qpois, test="F")
Anova(glm.pois)[1,1]/Anova(glm.pois)[1,2]/sigma2
## [1] 2.107903
Deviance
## [1] 5.129141
lsat <- sum(dpois(counts,counts,log = TRUE))
lcur <- sum(dpois(counts,glm.pois$fitted.values,log = TRUE))
2*(lsat-lcur)
## [1] 5.129141
Deviance residuals
lsat.i <- dpois(counts,counts,log = TRUE)
lcur.i <- dpois(counts,glm.pois$fitted.values,log = TRUE)
e.dev <- sign(counts-glm.pois$fitted) * sqrt(2*(lsat.i-lcur.i))
e.dev
## 1 2 3 4 5 6
## -0.67124923 0.96272360 -0.16964662 -0.21998507 -0.95552353 1.04938637
## 7 8 9
## 0.84715368 -0.09167147 -0.96656372
resid(glm.pois,type="deviance")
## 1 2 3 4 5 6
## -0.67124923 0.96272360 -0.16964662 -0.21998507 -0.95552353 1.04938637
## 7 8 9
## 0.84715368 -0.09167147 -0.96656372
glm.pois.out.null <- glm(counts ~ treatment, family = poisson())
anova(glm.pois.out.null,glm.pois)
lrtfull <- logLik(glm.pois)
lrtout0 <- logLik(glm.pois.out.null)
2*(lrtfull-lrtout0)
## 'log Lik.' 5.452305 (df=5)
Approximate F-test
2
glm.qpois.out.null <- glm(counts ~ treatment, family = quasipoisson())
anova(glm.qpois,glm.qpois.out.null,test = "F")
## 'log Lik.' 5.452305 (df=5)
2*(lrtfull-lrtout0)/2/sigma2
## 'log Lik.' 2.107903 (df=5)
---
title: 'Quasi-likelihood'
author: "Lieven Clement"
date: "Last edited on `r format(Sys.time(), '%d %B, %Y')`"
output: 
  html_document:
    toc: true
    toc_float: true
  pdf_document:
    toc: true
    number_sections: true
    latex_engine: xelatex
always_allow_html: true
linkcolor: blue
urlcolor: blue 
citecolor: blue
link-citations: yes

---

# Exponential Family

$$
f(y_i\vert \theta_i,\phi)=\exp\left\{ \frac{y_i\theta_i- b(\theta_i)}{a(\phi)}+c(y_i,\phi)\right\}
$$

likelihood to observe $y_1, \ldots, y_n$ independent observations 
$$L(\boldsymbol{\theta},\phi\vert \boldsymbol{y})=\prod\limits_{i=1}^n f(y_i,\theta_i,\phi)$$

log-likelihood
$$
l(\boldsymbol{\theta},\phi\vert \boldsymbol{y}) =  \sum\limits_{i=1}^n \log  f(y_i,\theta_i,\phi)
$$

Log-likelihood for one observation: 
$$
l(\theta_i,\phi\vert y_i)=\left\{ \frac{y_i\theta_i- b(\theta_i)}{a(\phi)}+c(y_i,\phi)\right\}
$$

- $E[y_i]=\mu_i=b^\prime(\theta_i)$
- $\text{var}[y_i]=b^{\prime\prime}(\theta_i) a(\phi) =V(\mu_i)$

e.g. for Poisson data: 
$\text{var}[y_i] = \mu_i$ and for negative binomial data $\text{var}[y_i] = \mu_i + \phi \mu_i^2$.

## Parameter Estimation: Maximum Likelihood

$$
S(\boldsymbol{\beta}) = \frac{\partial  l(\boldsymbol{\mu} \vert \mathbf{y})}{
\partial{\boldsymbol{\beta}}} = 0
$$

$$
S_i(\boldsymbol{\beta})= \frac{y_i-\mu_i}{\text{var}[y_i]}\frac{\partial\mu}{\partial\eta}\mathbf{x}_i
$$


There are only two moments involved in the estimation equations of the mean model parameters: 
the mean and the variance! 

$$
S(\boldsymbol{\beta})=\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right) = 0
$$

We can solve this set of score equations iteratively to estimate the model parameters: 
$$
\mathbf{\beta}^{k+1} = (\mathbf{X}^T\mathbf{W}^k\mathbf{X})^{-1}\mathbf{X}^T\mathbf{W}^kz^{k}
$$

with  pseudodata 

$$
z^k_i = \eta^k_i + \left.\frac{\partial \eta_i}{\partial \mu_i}\right\vert_k (y_i - \mu^k_i) 
$$


# Quasi-likelihood 

We no longer define the full distribution but only two moments: the mean and the variance of $y_i$. 

- We typically define these based on an existing distribution.
- However we make the variance more flexible, i.e. we rescale it with an additional model parameter. 

- Hence, we can model data that are over or under disperse with respect to a known distribution. 

$$
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 V(\mu_i)
\end{array}\right.
$$


e.g. quasi poisson

$$
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 \mu_i
\end{array}\right.
$$

e.g. quasi-negative binomial

$$
\left\{ \begin{array}{rcl}
E[Y_i\vert x_i] &=& \mu_i\\
g(\mu_i) &=& \eta_i\\
\eta_i &=& \mathbf{x}_i^T\boldsymbol{\beta}\\
\text{var}[Y_i] &=& \sigma^2 (\mu_i + \phi \mu_i^2)
\end{array}\right.
$$

## Parameter Estimation

Note, that this leads to the following estimation equations:

$$
U_i(\boldsymbol{\beta})= \frac{y_i-\mu_i}{\sigma^2V(\mu_i)}\frac{\partial\mu}{\partial\eta}\mathbf{x}_i
$$
 

$$
\begin{array}{rcccc}
U(\boldsymbol{\beta})&=&\left[\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right)\right]/\sigma^2 &=& 0\\
&&\Updownarrow\\
&&\mathbf{X}^T\mathbf{A}\left(\mathbf{y}-\boldsymbol{\mu}\right) &=& 0
\end{array}
$$
Hence, the estimating equations for the mean model parameters remain the same as those for the conventional distribution where the quasi-likelihood is derived from. 

The variance covariance matrix of the mean model parameters then becomes: 
$$
\Sigma_{\hat{\boldsymbol{\beta}}}= (\mathbf{X}^T\mathbf{WX})^{-1}\sigma^2
$$

We can estimate $\sigma^2$ using a moment estimator on the residual vector $\mathbf{y}-\boldsymbol{\mu}$, i.e. 

$$
\hat{\sigma}^2 = \frac{1}{n-p} \sum_\limits{i=1}^n \frac{(y_i-\hat\mu_i)^2}{V(\hat\mu_i)}
$$



Note, that 
$$e_i^p=\frac{(y_i-\hat\mu_i)}{\sqrt{V(\hat\mu_i)}}$$ are also referred to as the Pearson residuals. 

Another type of residuals for GLMs are deviance residuals, i.e. 

$$e_i^d = \text{sign}(y_i-\hat\mu_i)\sqrt{2[l(y_i,y_i)-l(y_i,\hat\mu_i)]}
$$
So another estimator is 

$$\hat{\sigma}^2 = \frac{\sum_\limits{i=1}^n(e_i^d)^2}{n-p} = \frac{D}{n-p}
$$
with D the deviance statistic: the LRT test between the saturated model (a model that provides a perfect fit) and the current model:

$$
D = 2 \sum\limits_{i=1}^n [l(y_i,y_i,\phi)- l(y_i,\hat{\mu}_i,\phi)]
$$

So the standard errors on the model parameters under quasi-likelihood become: 

$$
\hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{QL} = \hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{ML}\times \hat{\sigma}$$

## Hypothesis tests

An approximate t-test statistic can be defined as

$$
t = \frac{\mathbf{L}^T\hat{\boldsymbol{\beta}}}{\hat{\text{se}}_{\mathbf{L}^T\hat{\boldsymbol{\beta}}}^{QL}} \approx t_{n-p}\vert H_0
$$

And an approximate F-test statistic can be defined as: 

$$F = \frac{\frac{\text{LRT}^{ML}}{c}}{\hat\sigma^2}  \approx F_{c,n-p} \vert H_0,$$
with c the degrees of freedom of the LRT statistic.

## Example 

```{r}
## quasipoisson.
counts <- c(18,17,15,20,10,20,25,13,12)
outcome <- gl(3,1,9)
treatment <- gl(3,3)
d.AD <- data.frame(treatment, outcome, counts)
d.AD
```

```{r}
glm.pois <- glm(counts ~ outcome + treatment, family = poisson())
summary(glm.pois)
```

```{r}
glm.qpois <- glm(counts ~ outcome+treatment, family = quasipoisson())
summary(glm.qpois)
```

Estimate dispersion ourselves? 
We first calculate the Pearson residuals. 

```{r}
ep <- (counts - glm.pois$fitted)/sqrt(glm.pois$fitted)
range(ep - resid(glm.pois,type="pearson"))
```

Now, we can estimate the quasi-dispersion parameter
```{r}
n <- length(counts)
p <- length(coef(glm.pois))
sigma2 <- sum(ep^2)/(n-p)
sigma2
```

```{r}
poisRes <- summary(glm.pois)$coef
poisRes
qlRes <- summary(glm.qpois)$coef
qlRes
cbind(ql.se=qlRes[,2],pois.se=poisRes[,2],qlself.se=poisRes[,2]*sqrt(sigma2))
```

### Approximate F-test

LR -test with Poisson regression: 

```{r}
library(car)
Anova(glm.pois)
```
We check that the approximate F-statistic equals LRT/df/sigma2 

```{r}
Anova(glm.qpois, test="F")
Anova(glm.pois)[1,1]/Anova(glm.pois)[1,2]/sigma2
```


### Deviance

```{r}
deviance(glm.pois)
lsat <- sum(dpois(counts,counts,log = TRUE))
lcur <- sum(dpois(counts,glm.pois$fitted.values,log = TRUE))
2*(lsat-lcur)
```

Deviance residuals

```{r}
lsat.i <-  dpois(counts,counts,log = TRUE)
lcur.i <- dpois(counts,glm.pois$fitted.values,log = TRUE)
e.dev <- sign(counts-glm.pois$fitted) * sqrt(2*(lsat.i-lcur.i))
e.dev
resid(glm.pois,type="deviance")
```

```{r}
glm.pois.out.null <- glm(counts ~  treatment, family = poisson())
anova(glm.pois.out.null,glm.pois)
lrtfull <- logLik(glm.pois)
lrtout0 <- logLik(glm.pois.out.null)
2*(lrtfull-lrtout0)
```

### Approximate F-test 2

```{r}
glm.qpois.out.null <- glm(counts ~  treatment, family = quasipoisson())
anova(glm.qpois,glm.qpois.out.null,test = "F")
2*(lrtfull-lrtout0)
2*(lrtfull-lrtout0)/2/sigma2
```
