## 4.5 Inference for model parameters

The assumptions on which the logistic model is constructed allow to specify what is the *asymptotic* distribution of the *random vector* \(\hat{\boldsymbol{\beta}}\). Again, the distribution is derived conditionally on the sample predictors \(\mathbf{X}_1,\ldots,\mathbf{X}_n\). In other words, we assume that the randomness of \(Y\) comes only from \(Y|(X_1=x_1,\ldots,X_k=x_k)\sim\mathrm{Ber}(p(\mathbf{x}))\) and not from the predictors. To denote this, we employ lowercase for the sample predictors \(\mathbf{x}_1,\ldots,\mathbf{x}_n\).

There is an important difference between the inference results for the linear model and for logistic regression:

**In linear regression the inference is exact**. This is due to the nice properties of the normal, least squares estimation and linearity. As a consequence, the distributions of the coefficients are perfectly known assuming that the assumptions hold.**In logistic regression the inference is asymptotic**. This means that the distributions of the coefficients are unknown except for large sample sizes \(n\), for which we have**approximations**. The reason is the more complexity of the model in terms of non-linearity. This is the usual situation for the majority of the regression models.

### 4.5.1 Distributions of the fitted coefficients

The distribution of \(\hat{\boldsymbol{\beta}}\) is given by the asymptotic theory of MLE: \[\begin{align} \hat{\boldsymbol{\beta}}\sim\mathcal{N}_{k+1}\left(\boldsymbol{\beta},I(\hat{\boldsymbol{\beta}})^{-1}\right) \tag{4.10} \end{align}\] where \(\sim\) must be understood as*approximately distributed as […] when \(n\to\infty\)*for the rest of this chapter. \(I(\boldsymbol{\beta})\) is known as the

*Fisher information matrix*, and receives that name because

*it measures the information available in the sample for estimating \(\boldsymbol{\beta}\)*. Therefore, the

*larger*the matrix is, the more precise is the estimation of \(\boldsymbol{\beta}\), because that results in smaller variances in (4.10). The inverse of the Fisher information matrix is \[\begin{align} I(\hat{\boldsymbol{\beta}})^{-1}=(\mathbf{X}^T\mathbf{V}\mathbf{X})^{-1}, \tag{4.11} \end{align}\]

where \(\mathbf{V}\) is a diagonal matrix containing the *different* variances for each \(Y_i\) (remember that \(p(\mathbf{x})=1/(1+e^{-(\beta_0+\beta_1x_1+\ldots+\beta_kx_k)})\)): \[
\mathbf{V}=\begin{pmatrix}
p(\mathbf{X}_1)(1-p(\mathbf{X}_1)) & & &\\
& p(\mathbf{X}_2)(1-p(\mathbf{X}_2)) & & \\
& & \ddots & \\
& & & p(\mathbf{X}_n)(1-p(\mathbf{X}_n))
\end{pmatrix}
\] In the case of the multiple linear regression, \(I(\hat{\boldsymbol{\beta}})^{-1}=\sigma^2(\mathbf{X}^T\mathbf{X})^{-1}\) (see (3.6)), so the presence of \(\mathbf{V}\) here is revealing the heteroskedasticity of the model.

The interpretation of (4.10) and (4.11) give some useful insights on what concepts affect the quality of the estimation:

**Bias**. The estimates are*asymptotically*unbiased.**Variance**. It depends on:*Sample size \(n\)*. Hidden inside \(\mathbf{X}^T\mathbf{V}\mathbf{X}\). As \(n\) grows, the precision of the estimators increases.*Weighted predictor sparsity \((\mathbf{X}^T\mathbf{V}\mathbf{X})^{-1}\)*. The more*sparse*the predictor is (small \(|(\mathbf{X}^T\mathbf{V}\mathbf{X})^{-1}|\)), the more precise \(\hat{\boldsymbol{\beta}}\) is.

**The precision of \(\hat{\boldsymbol{\beta}}\) is affected by the value of \(\boldsymbol{\beta}\)**, which is hidden inside \(\mathbf{V}\). This contrasts sharply with the linear model, where the precision of the least squares estimator was not affected by the value of the unknown coefficients (see (3.6)). The reason is partially due to the

**heteroskedasticity**of logistic regression, which implies a dependence of the variance of \(Y\) in the logistic curve, hence in \(\boldsymbol{\beta}\).

*\(\mathbf{V}\) is unknown*in practice because it depends on \(\boldsymbol{\beta}\). Plugging-in the estimate \(\hat{\boldsymbol{\beta}}\) to \(\boldsymbol{\beta}\) in \(\mathbf{V}\) results in \(\hat{\mathbf{V}}\). Now we can use \(\hat{\mathbf{V}}\) to get \[\begin{align} \frac{\hat\beta_j-\beta_j}{\hat{\mathrm{SE}}(\hat\beta_j)}\sim \mathcal{N}(0,1),\quad\hat{\mathrm{SE}}(\hat\beta_j)^2=v_j^2\tag{4.12} \end{align}\]

where \[
v_j\text{ is the }j\text{-th element of the diagonal of }(\mathbf{X}^T\hat{\mathbf{V}}\mathbf{X})^{-1}.
\] The LHS of (3.7) is the **Wald statistic** for \(\beta_j\), \(j=0,\ldots,k\). They are employed for building confidence intervals and hypothesis tests.

### 4.5.2 Confidence intervals for the coefficients

Thanks to (4.12), we can have the \(100(1-\alpha)\%\) CI for the coefficient \(\beta_j\), \(j=0,\ldots,k\): \[\begin{align} \left(\hat\beta_j\pm\hat{\mathrm{SE}}(\hat\beta_j)z_{\alpha/2}\right)\tag{4.13} \end{align}\]where \(z_{\alpha/2}\) is the *\(\alpha/2\)-upper quantile of the \(\mathcal{N}(0,1)\)*. In case we are interested in the CI for \(e^{\beta_j}\), we can just simply take the exponential on the above CI. So the \(100(1-\alpha)\%\) CI for \(e^{\beta_j}\), \(j=0,\ldots,k\), is \[
e^{\left(\hat\beta_j\pm\hat{\mathrm{SE}}(\hat\beta_j)z_{\alpha/2}\right)}.
\] Of course, this CI is **not** the same as \(\left(e^{\hat\beta_j}\pm e^{\hat{\mathrm{SE}}(\hat\beta_j)z_{\alpha/2}}\right)\), which is not a CI for \(e^{\hat\beta_j}\).

Let’s see how we can compute the CIs. We return to the `challenger`

dataset, so in case you do not have it loaded, you can download it here. We analyze the CI for the coefficients of `fail.field ~ temp`

.

```
# Fit model
nasa <- glm(fail.field ~ temp, family = "binomial", data = challenger)
# Confidence intervals at 95%
confint(nasa)
## Waiting for profiling to be done...
## 2.5 % 97.5 %
## (Intercept) 1.3364047 17.7834329
## temp -0.9237721 -0.1089953
# Confidence intervals at other levels
confint(nasa, level = 0.90)
## Waiting for profiling to be done...
## 5 % 95 %
## (Intercept) 2.2070301 15.7488590
## temp -0.8222858 -0.1513279
# Confidence intervals for the factors affecting the odds
exp(confint(nasa))
## Waiting for profiling to be done...
## 2.5 % 97.5 %
## (Intercept) 3.8053375 5.287456e+07
## temp 0.3970186 8.967346e-01
```

In this example, the 95% confidence interval for \(\beta_0\) is \((1.3364, 17.7834)\) and for \(\beta_1\) is \((-0.9238, -0.1090)\). For \(e^{\beta_0}\) and \(e^{\beta_1}\), the CIs are \((3.8053, 5.2874\times10^7)\) and \((0.3070, 0.8967)\), respectively. Therefore, we can say with a 95% confidence that:

- When
`temp`

=0, the probability of`fail.field`

=1 is significantly lager than the probability of`fail.field`

=0 (using the CI for \(\beta_0\)). Indeed,`fail.field`

=1 is between \(3.8053\) and \(5.2874\times10^7\) more likely than`fail.field`

=0 (using the CI for \(e^{\beta_0}\)). `temp`

has a significantly negative effect in the probability of`fail.field`

=1 (using the CI for \(\beta_1\)). Indeed, each unit increase in`temp`

produces a reduction of the odds of`fail.field`

by a factor between \(0.3070\) and \(0.8967\) (using the CI for \(e^{\beta_1}\)).

Compute and interpret the CIs for the exponentiated coefficients, at level \(\alpha=0.05\), for the following regressions (`challenger`

dataset):

`fail.field ~ temp + pres.field`

`fail.nozzle ~ temp + pres.nozzle`

`fail.field ~ temp + pres.nozzle`

`fail.nozzle ~ temp + pres.field`

### 4.5.3 Testing on the coefficients

The distributions in (4.12) also allow to conduct a formal hypothesis test on the coefficients \(\beta_j\), \(j=0,\ldots,k\). For example, the test for significance: \[\begin{align*} H_0:\beta_j=0 \end{align*}\] for \(j=0,\ldots,k\). The test of \(H_0:\beta_j=0\) with \(1\leq j\leq k\) is specially interesting, since it allows to answer whether*the variable \(X_j\) has a significant effect on \(\mathbb{P}[Y=1]\)*. The statistic used for testing for significance is the Wald statistic \[\begin{align*} \frac{\hat\beta_j-0}{\hat{\mathrm{SE}}(\hat\beta_j)}, \end{align*}\]

which is asymptotically distributed as a \(\mathcal{N}(0,1)\) *under the (veracity of) the null hypothesis*. \(H_0\) is tested *against* the *bilateral* alternative hypothesis \(H_1:\beta_j\neq 0\).

The tests for significance are built-in in the `summary`

function. However, a note of caution is required when applying the rule of thumb:

Is the CI for \(\beta_j\) below (above) \(0\) at level \(\alpha\)?

- Yes \(\rightarrow\) reject \(H_0\) at level \(\alpha\).
- No \(\rightarrow\) the criterion is not conclusive.

The significances given in `summary`

and the output of `confint`

are *slightly* incoherent and the previous rule of thumb **does not apply**. The reason is because `MASS`

’s `confint`

is using a more sophisticated method (profile likelihood) to estimate the standard error of \(\hat\beta_j\), \(\hat{\mathrm{SE}}(\hat\beta_j)\), and not the asymptotic distribution behind Wald statistic.

By changing `confint`

to `R`

’s default `confint.default`

, the results of the latter will be completely equivalent to the significances in `summary`

, and the rule of thumb still be completely valid. For the contents of this course we prefer `confint.default`

due to its better interpretability.

To illustrate this we consider the regression of `fail.field ~ temp + pres.field`

:

```
# Significances with asymptotic approximation for the standard errors
nasa2 <- glm(fail.field ~ temp + pres.field, family = "binomial",
data = challenger)
summary(nasa2)
##
## Call:
## glm(formula = fail.field ~ temp + pres.field, family = "binomial",
## data = challenger)
##
## Deviance Residuals:
## Min 1Q Median 3Q Max
## -1.2109 -0.6081 -0.4292 0.3498 2.0913
##
## Coefficients:
## Estimate Std. Error z value Pr(>|z|)
## (Intercept) 6.642709 4.038547 1.645 0.1000
## temp -0.435032 0.197008 -2.208 0.0272 *
## pres.field 0.009376 0.008821 1.063 0.2878
## ---
## Signif. codes: 0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
##
## (Dispersion parameter for binomial family taken to be 1)
##
## Null deviance: 28.267 on 22 degrees of freedom
## Residual deviance: 19.078 on 20 degrees of freedom
## AIC: 25.078
##
## Number of Fisher Scoring iterations: 5
# CIs with asymptotic approximation - coherent with summary
confint.default(nasa2, level = 0.90)
## 5 % 95 %
## (Intercept) -0.000110501 13.28552771
## temp -0.759081468 -0.11098301
## pres.field -0.005132393 0.02388538
confint.default(nasa2, level = 0.99)
## 0.5 % 99.5 %
## (Intercept) -3.75989977 17.04531697
## temp -0.94249107 0.07242659
## pres.field -0.01334432 0.03209731
# CIs with profile likelihood - incoherent with summary
confint(nasa2, level = 0.90) # intercept still significant
## Waiting for profiling to be done...
## 5 % 95 %
## (Intercept) 0.945372123 14.93392497
## temp -0.845250023 -0.16532086
## pres.field -0.004184814 0.02602181
confint(nasa2, level = 0.99) # temp still significant
## Waiting for profiling to be done...
## 0.5 % 99.5 %
## (Intercept) -1.86541750 21.49637422
## temp -1.17556090 -0.04317904
## pres.field -0.01164943 0.03836968
```

For the previous exercise, check the differences of using `confint`

or `confint.default`

for computing the CIs.