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Weak Instruments · Tutorial 563 of 972

Worked Weak-Instrument Analysis of a Just-Identified Model

Work through a just-identified instrumental-variables example to see how weak first-stage evidence can make conventional Wald inference much narrower than Anderson–Rubin inference.

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What You'll Learn

  • Identify the structural and first-stage equations in a just-identified IV model
  • Calculate the first-stage F statistic and partial R-squared from numerical summaries
  • Derive a conventional Wald interval using the covariance of reduced-form estimates
  • Construct and interpret an Anderson–Rubin test by inverting its acceptance condition
  • Compare the two confidence sets without treating a first-stage diagnostic as proof of instrument validity

Why Work Through a Numerical Example?

In a just-identified instrumental-variables model, one instrument is used for one endogenous regressor. The estimator is easy to express as a ratio of two reduced-form estimates. That simplicity can be misleading: when the first stage is weak, the ratio can be highly variable, and conventional Wald inference can give a very different impression from inference based on the Anderson–Rubin test.

This worked analysis follows one numerical example from first-stage diagnosis to confidence-set interpretation. The calculations use a large-sample normal approximation for the reduced-form estimates. They illustrate the contrast between the methods; they do not establish that an instrument is valid. Instrument relevance, instrument exogeneity, and the exclusion restriction are distinct assumptions.

Model and Numerical Summary

Consider the structural equation \(y_i=\alpha+\beta x_i+u_i\), where \(x_i\) is endogenous, and use an instrument \(z_i\). The first-stage equation relates \(x_i\) to an intercept and \(z_i\). There is one excluded instrument and one endogenous regressor, so the model is just identified. For the calculations below, the intercept is included and all reported reduced-form estimates are understood to use the same sample.

Let \(\hat\pi\) be the estimated first-stage coefficient of \(z_i\) in the regression for \(x_i\). Let \(\hat\gamma_y\) be the reduced-form coefficient of \(z_i\) in the regression for \(y_i\). In a just-identified model, the IV estimate is the ratio \(\hat\gamma_y/\hat\pi\), provided \(\hat\pi\ne 0\).

Definition: The first-stage F statistic tests the null that the excluded instrument has zero coefficient in the first-stage regression. With one excluded instrument and the conventional homoskedastic standard error, \(F=t^2\), where \(t\) is the first-stage coefficient divided by its standard error. The partial R-squared is the fraction of the variation in the endogenous regressor left after accounting for included regressors that is explained by the excluded instrument.

Suppose \(n=100\), with no included regressors other than an intercept. The first-stage estimate is \(\hat\pi=0.20\), with standard error \(0.10\). The reduced-form estimates and their estimated covariance matrix are

$$ \hat\gamma_y=0.30,\qquad \widehat{\operatorname{Var}} \begin{pmatrix} \hat\gamma_y\\ \hat\pi \end{pmatrix} = \begin{pmatrix} 0.0144 & 0.0060\\ 0.0060 & 0.0100 \end{pmatrix}. $$

Thus the reduced-form standard errors are \(0.12\) and \(0.10\), and the estimated correlation is \(0.006/(0.12\times0.10)=0.5\). The covariance matrix is positive definite: its determinant is \(0.0144(0.0100)-0.0060^2=0.000108>0\). This summary will be used consistently in both forms of inference.

First-Stage Strength

Worked Example: Calculating F and Partial R-Squared

The first-stage t statistic is the coefficient estimate divided by its standard error:

$$ t=\frac{0.20}{0.10}=2,\qquad F=t^2=2^2=4. $$

The first-stage regression has \(100-2=98\) residual degrees of freedom: one intercept and one instrument are estimated. With one excluded instrument, the partial R-squared and F statistic obey \(F=R^2_{\mathrm{partial}}/(1-R^2_{\mathrm{partial}})\times98\). Solving for the partial R-squared gives

$$ R^2_{\mathrm{partial}}=\frac{F}{F+98} =\frac{4}{102}\approx0.0392. $$

So the instrument explains about \(3.9\%\) of the variation in \(x_i\) remaining after the intercept is accounted for. The F statistic and partial R-squared describe first-stage relevance in this sample; neither verifies instrument exogeneity or the exclusion restriction.

An F statistic of 4 is a warning that the first stage is not strong in this example. It is useful to report the number and the partial R-squared rather than converting either into a claim that identification has been established or disproved. A weak first stage matters especially because the IV estimate divides by \(\hat\pi\).

Conventional Wald Inference

The just-identified IV estimate is the ratio of the reduced-form coefficients:

$$ \hat\beta_{\mathrm{IV}}=\frac{\hat\gamma_y}{\hat\pi} =\frac{0.30}{0.20}=1.50. $$

A conventional Wald interval uses an approximately normal distribution for the estimator. Applying the delta method to the ratio \(g(a,b)=a/b\) gives gradient \((1/b,-a/b^2)\). Evaluated at the estimates, this is \((1/\hat\pi,-\hat\beta_{\mathrm{IV}}/\hat\pi)\). Therefore the estimated variance is

$$ \widehat{\operatorname{Var}}(\hat\beta_{\mathrm{IV}}) = \frac{ \widehat{\operatorname{Var}}(\hat\gamma_y) +\hat\beta_{\mathrm{IV}}^2\widehat{\operatorname{Var}}(\hat\pi) -2\hat\beta_{\mathrm{IV}}\widehat{\operatorname{Cov}}(\hat\gamma_y,\hat\pi) }{\hat\pi^2}. $$

This expression uses both variances and their covariance; omitting the covariance would not be the delta-method variance for the ratio. In the example, the numerator is \(0.0144+(1.50)^2(0.0100)-2(1.50)(0.0060)=0.0189\). Hence

$$ \widehat{\operatorname{Var}}(\hat\beta_{\mathrm{IV}}) =\frac{0.0189}{0.20^2}=0.4725,\qquad \widehat{\operatorname{SE}}(\hat\beta_{\mathrm{IV}})=\sqrt{0.4725}\approx0.6874. $$

Worked Example: Forming the Conventional Wald Interval

Using the two-sided 95% normal critical value \(1.96\), the Wald interval is

$$ 1.50\pm1.96(0.6874) =1.50\pm1.3473 \approx[0.153,\,2.847]. $$

Under this approximation, the conventional interval excludes zero and appears relatively concentrated around \(1.50\). But this calculation relies on a normal approximation for a ratio whose denominator, the first-stage estimate, is imprecise. With a weak first stage, the ratio can have a sampling distribution poorly represented by a normal curve, so a conventional Wald interval can be misleadingly reassuring.

Anderson–Rubin Test and Inversion

For a proposed structural value \(\beta_0\), form the outcome \(y_i-\beta_0x_i\) and test whether the instrument's reduced-form coefficient for that outcome is zero. In terms of the estimates above, that coefficient is \(\hat\gamma_y-\beta_0\hat\pi\). Its estimated variance is obtained from the same covariance matrix:

$$ \widehat{\operatorname{Var}}(\hat\gamma_y-\beta_0\hat\pi) =0.0144+\beta_0^2(0.0100)-2\beta_0(0.0060). $$

The Anderson–Rubin statistic in this one-instrument example is the absolute value of that coefficient divided by its standard error. Under the null hypothesis that \(\beta=\beta_0\), and assuming the instrument is valid, the reduced-form coefficient being tested is zero. If the reduced-form estimates are approximately jointly normal with the stated covariance, this standardized linear combination is approximately standard normal under the null. Rejecting when its absolute value exceeds \(1.96\) gives an approximately 5% two-sided test.

This explains the weak-instrument robustness of the test: its null statistic tests a reduced-form restriction and does not divide by \(\hat\pi\). Under the stated approximation, its null calibration does not require a strong first stage. Inverting the test means retaining every value \(\beta_0\) that is not rejected.

Worked Example: Inverting the Anderson–Rubin Test

For a 95% confidence set, retain \(\beta_0\) when

$$ (0.30-0.20\beta_0)^2 \leq 1.96^2\bigl(0.0144+0.0100\beta_0^2-0.0120\beta_0\bigr). $$

Since \(1.96^2=3.8416\), moving the right-hand side to the left gives

$$ 0.001584\beta_0^2-0.0739008\beta_0+0.03468096\leq0. $$

The quadratic coefficient is positive. Its roots are approximately \(0.474\) and \(46.18\): the discriminant is approximately \(0.0052416\), its square root is approximately \(0.072399\), and the quadratic formula divides \(0.0739008\pm0.072399\) by \(2(0.001584)=0.003168\). A positive-leading-coefficient quadratic is nonpositive between its two real roots. The Anderson–Rubin confidence set is therefore approximately

$$ [0.474,\,46.18]. $$

For a direct check, at \(\beta_0=0\) the statistic is \(0.30/0.12=2.50\), which exceeds \(1.96\), so zero is rejected. At \(\beta_0=1.50\), the numerator is \(0.30-1.50(0.20)=0\), so that value is retained. The very large upper endpoint shows how little precision the data provide about some structural values despite the much narrower Wald interval.

What the Comparison Tells Us

FeatureConventional WaldAnderson–Rubin
Numerical result hereApproximately [0.153, 2.847]Approximately [0.474, 46.18]
Core calculationRatio estimate and its estimated standard errorTest of the reduced-form coefficient for \(y-\beta_0x\)
Response to a weak first stageCan be poorly approximated by a normal intervalNull test does not divide by the first-stage estimate

The Anderson–Rubin set is much wider here. That width is not a computational defect: it reflects the limited information in a weak first stage about the structural coefficient. In other data, inversion can produce an unbounded or disconnected set; the shape follows from the test inequality and should be reported rather than forced into the form of a familiar symmetric interval.

Neither calculation establishes the causal interpretation of \(\hat\beta_{\mathrm{IV}}\). A weak-instrument-robust test addresses the reliability of inference about \(\beta\) under the model's assumptions; it does not repair an invalid instrument. Likewise, a first-stage diagnostic describes relevance, not exogeneity. The substantive justification for the instrument remains essential.

Common Mistake

Wrong reasoning: “The first-stage t statistic is 2, so the instrument is strong enough; the Wald interval is narrower, so it must be the more informative answer.” This treats one diagnostic as a pass/fail guarantee and mistakes narrowness for reliable precision.

Correction: The first-stage evidence here is \(F=4\) and partial \(R^2\approx0.0392\). These numbers indicate limited relevance in the sample, so the ratio-based Wald approximation deserves caution. The Anderson–Rubin set, calculated by testing each candidate value without dividing by the first-stage estimate, reveals that uncertainty is much larger. Report the method and assumptions, and interpret the contrast rather than selecting the narrower result by default.

Check Your Understanding

Use the numerical summary in this tutorial to answer the following.

  1. Why is the conventional first-stage F statistic equal to the square of the first-stage t statistic in this one-instrument example?
  2. How does the first-stage partial R-squared follow from \(F=4\) and 98 residual degrees of freedom?
  3. Which covariance term enters the delta-method variance of the IV ratio, and what would go wrong if it were omitted?
  4. Why does the Anderson–Rubin test avoid dividing by the estimated first-stage coefficient?
  5. What does the much wider Anderson–Rubin confidence set indicate, and what important question about instrument validity does it not answer?
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