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Profile Likelihood and Intervals · Tutorial 289 of 981

Why Profile Intervals Are Often Asymmetric

See how likelihood shape, rather than a constant standard error, can make the two sides of a profile interval differ.

Advanced 11 min read

What You'll Learn

  • Define profile likelihood and compare its likelihood-ratio interval with a Wald interval.
  • Explain how changing curvature and a nonzero third derivative produce asymmetric endpoints.
  • Work through a sparse binomial logistic-regression coefficient and check its interval calculations.
  • Identify when a quadratic approximation makes a profile interval look symmetric.
  • Distinguish interval shape from the accuracy of its nominal coverage.

Why Compare the Two Kinds of Interval?

A Wald interval uses the estimated coefficient and its estimated standard error to place equal distances on either side of the estimate. A likelihood-ratio profile interval instead finds the coefficient values whose likelihood is not too far below its maximum. These procedures can give different answers when the log-likelihood is noticeably curved differently on its two sides.

This is especially visible with sparse binomial data. When the observed number of events is small, plausible probabilities can extend a long way toward zero, while the likelihood may fall more sharply in the other direction. On the logit scale, that unequal shape can yield unequal endpoint distances. The comparison below isolates this effect in a one-coefficient logistic regression.

Definition: Let \(\beta\) be a scalar target parameter, and let \(\lambda\) denote any nuisance parameters. The profile log-likelihood is \(\ell_p(\beta)=\max_{\lambda}\ell(\beta,\lambda)\), with the maximum taken over the allowed nuisance-parameter values. A likelihood-ratio profile confidence set with cutoff \(c\) is the set of \(\beta\) satisfying \(2\{\ell_p(\hat{\beta})-\ell_p(\beta)\}\leq c\), where \(\hat{\beta}\) maximizes the profile log-likelihood. A Wald interval has the form \(\hat{\beta}\pm z_{1-\alpha/2}\widehat{\operatorname{se}}(\hat{\beta})\).

The Wald formula is symmetric by construction: it uses one standard error at the estimate for both directions. A profile interval need not be symmetric because it follows the likelihood’s actual shape. For a nominal 95% likelihood-ratio interval in a regular one-parameter setting, the usual large-sample cutoff is \(c=\chi^2_{1,0.95}\approx3.8415\). This asymptotic cutoff does not guarantee exact 95% coverage in a small or sparse sample; interval shape and coverage calibration are separate issues.

A Sparse Binomial Logistic-Regression Example

Consider a binomial response \(Y\sim\operatorname{Binomial}(10,p)\) with two observed successes. Fit the logistic regression model \(\operatorname{logit}(p)=\beta x\), with the covariate \(x=1\) for this group and no intercept. Thus \(\beta\) is the group’s log odds, and the model has one coefficient. This deliberately simple setup makes the likelihood shape visible without introducing a nuisance parameter.

Worked Example: Profile and Wald Intervals With Two Events

The likelihood, apart from a factor that does not depend on \(\beta\), is \(L(\beta)\propto p^2(1-p)^8\), where \(p=\operatorname{logit}^{-1}(\beta)\). The log-likelihood is \(\ell(\beta)=2\beta-10\log(1+e^\beta)\). Its maximum occurs at \(\hat p=2/10=0.2\), so \(\hat\beta=\log(0.2/0.8)=\log(0.25)\approx-1.3863\).

For a candidate probability \(p\), twice the log-likelihood drop from the maximum is the binomial likelihood-ratio statistic \(q(p)=2\left\{2\log(0.2/p)+8\log(0.8/(1-p))\right\}\). Solving \(q(p)=3.8415\) gives approximate endpoints \(p_L\approx0.03636\) and \(p_U\approx0.49944\). Substituting these probabilities into the logit gives \(\beta_L=\log(0.03636/0.96364)\approx-3.2772\) and \(\beta_U=\log(0.49944/0.50056)\approx-0.0022\). Thus the profile interval is approximately \([-3.2772,-0.0022]\).

The endpoint distances from \(\hat\beta\) are about \(1.8909\) downward and \(1.3841\) upward. They are not equal. In contrast, the estimated standard error from the observed information is \(\widehat{\operatorname{se}}(\hat\beta)=\{10(0.2)(0.8)\}^{-1/2}=1/\sqrt{1.6}\approx0.7906\). The Wald interval is therefore \(-1.3863\pm1.96(0.7906)=[-2.9358,0.1632]\), to four decimal places. Its half-width is \(1.5495\) on each side. The profile interval is not merely a wider version of this interval: its lower endpoint is farther from the estimate, while its upper endpoint is closer.

The probability-scale endpoints help explain the imbalance. The data estimate a success probability of 0.2, but the likelihood-ratio set reaches down to about 0.036 and up to about 0.499. The logit transformation expresses those values as coefficients, but the main point here is the shape of the likelihood around its maximum: equal changes in \(\beta\) in opposite directions do not produce equal likelihood drops.

Curvature Explains Local Symmetry; Skewness Explains Its Failure

The local curvature at the maximum determines the Wald standard error. If the profile log-likelihood were exactly quadratic, its likelihood-ratio interval would be symmetric and would agree with the Wald interval when both use the same cutoff. The following result makes that comparison precise.

Result: Suppose \(\ell_p\) has an interior maximum at \(\hat\beta\), is twice continuously differentiable near \(\hat\beta\), and \(\ell_p''(\hat\beta)=-J\) for \(J>0\). Then, for \(\delta\) near zero, \(2\{\ell_p(\hat\beta)-\ell_p(\hat\beta+\delta)\}=J\delta^2+o(\delta^2)\). Consequently, the local likelihood-ratio endpoints for a small cutoff \(c>0\) are approximately \(\hat\beta\pm\sqrt{c/J}\). If the observed information is \(J\), the corresponding Wald half-width using cutoff \(c=z^2\) is \(z/\sqrt{J}\).

Proof. Since \(\hat\beta\) is an interior differentiable maximum, \(\ell_p'(\hat\beta)=0\). Taylor’s theorem gives \(\ell_p(\hat\beta+\delta)=\ell_p(\hat\beta)+\ell_p'(\hat\beta)\delta+\tfrac12\ell_p''(\hat\beta)\delta^2+o(\delta^2)\). Substituting the zero first derivative and \(\ell_p''(\hat\beta)=-J\) yields \(2\{\ell_p(\hat\beta)-\ell_p(\hat\beta+\delta)\}=J\delta^2+o(\delta^2)\). Ignoring the smaller-order remainder gives \(J\delta^2=c\), whose two solutions are \(\delta=\pm\sqrt{c/J}\). For a Wald interval, the local standard error is \(1/\sqrt J\), so the half-width is \(z/\sqrt J\). \(\square\)

This result describes a local approximation, not a promise of symmetry at every confidence level. To see the first term that can break the symmetry, suppose additionally that \(\ell_p\) has four continuous derivatives near \(\hat\beta\), and write \(K=\ell_p'''(\hat\beta)\). Taylor expansion gives \(2\{\ell_p(\hat\beta)-\ell_p(\hat\beta+\delta)\}=J\delta^2-\tfrac{K}{3}\delta^3+O(\delta^4)\). The cubic term changes sign when \(\delta\) changes sign. If the two nearby endpoints for a small cutoff \(c\) are written as \(\delta_s=s h+a h^2+O(h^3)\), where \(s\in\{-1,1\}\) and \(h=\sqrt{c/J}\), substitution gives \(2Ja-K/3=0\). Hence \(a=K/(6J)\), and \(\delta_s=s\sqrt{c/J}+\frac{K}{6J}\frac{c}{J}+O(c^{3/2})\).

Derivation of the endpoint expansion. In the likelihood-ratio expansion, the quadratic term contributes \(J\delta_s^2=c+2Js a h^3+O(h^4)\), and the cubic term contributes \(-\tfrac K3\delta_s^3=-\tfrac K3s h^3+O(h^4)\). For the likelihood-ratio value to equal \(c\), the coefficient of \(s h^3\) must vanish: \(2Ja-K/3=0\). This gives \(a=K/(6J)\) and the stated expansion. Both endpoints receive the same second-order displacement from the maximum, which makes their distances unequal. \(\square\)

For the sparse example, \(\ell''(\hat\beta)=-10(0.2)(0.8)=-1.6\), so \(J=1.6\). Also \(\ell'''(\hat\beta)=-10(0.2)(0.8)(1-2(0.2))=-0.96\). With \(c=3.8415\), the quadratic half-width is \(\sqrt{c/1.6}\approx1.5495\). The cubic approximation shifts both endpoints by \(\frac{-0.96}{6(1.6)}(1.5495)^2\approx-0.2401\), predicting displacements of roughly \(-1.7896\) and \(1.3094\). This small-cutoff expansion is only approximate at a 95% cutoff, but it correctly predicts the direction of the asymmetry: the negative third derivative shifts both endpoints toward smaller coefficients.

Worked Example: A Balanced Binomial Contrast

Now let \(Y\sim\operatorname{Binomial}(8,p)\) and observe \(Y=4\) in the same model \(\operatorname{logit}(p)=\beta\). The estimate is \(\hat p=0.5\) and \(\hat\beta=0\). For a candidate probability, the likelihood-ratio statistic is \(q(p)=8\log\{0.25/[p(1-p)]\}\). Setting this equal to \(3.8415\) gives \(p(1-p)=0.25e^{-3.8415/8}\approx0.1547\).

Solving the quadratic gives \(p_L\approx0.1912\) and \(p_U\approx0.8088\). These probabilities are complements, so their logits are opposites: \(\beta_L\approx-1.442\) and \(\beta_U\approx1.442\). Here the profile interval is symmetric. The balanced likelihood has this symmetry around \(\beta=0\); symmetry is possible, but it is not a general feature of profile intervals.

Worked Example: Checking the Local Curvature Approximation

For the two-event example, the local curvature gives \(J=1.6\), and the Wald 95% half-width is \(1.96/\sqrt{1.6}\approx1.5495\). A purely quadratic log-likelihood would therefore put the endpoints at \(-1.3863-1.5495=-2.9358\) and \(-1.3863+1.5495=0.1632\). These are exactly the Wald endpoints, by construction.

The profile endpoints, about \(-3.2772\) and \(-0.0022\), differ because the actual likelihood does not remain quadratic over displacements of this size. The cubic calculation predicts a shift in the negative direction, and the full profile calculation confirms that the lower endpoint is farther from the estimate than the upper one. The expansion explains the mechanism; solving the full likelihood equation supplies the interval.

Interpretation and Common Pitfalls

A profile interval uses the likelihood over the range of candidate values, whereas a Wald interval summarizes the likelihood locally through curvature at its maximum. The profile approach can therefore retain information about asymmetry that a single standard error cannot express. In a regression analysis, this can matter when a coefficient is estimated from sparse events or when plausible values span a region where the likelihood changes curvature substantially.

Asymmetry alone does not establish that a profile interval has better coverage, nor does it show that the Wald interval is always unsuitable. The cutoff’s calibration, the model assumptions, and the amount of information in the data also matter. In particular, the chi-square cutoff used here is an asymptotic approximation; with sparse data, its nominal coverage may be imperfect.

  • Mistake: assuming every interval must be centered on the estimate. That is true of the usual Wald construction, but not of a likelihood-ratio interval. Check the two profile endpoints rather than forcing them into a symmetric form.
  • Mistake: treating the local quadratic approximation as the full likelihood. Curvature describes behavior near the maximum. If an endpoint is far away, higher-order terms can materially change its location.
  • Mistake: confusing shape with calibration. An asymmetric profile interval is not automatically an exact interval. The choice of likelihood-ratio cutoff and its finite-sample performance are separate questions.
  • Mistake: rounding an endpoint before transforming it and reporting false precision. If probabilities are displayed only approximately, coefficient endpoints computed from them should be reported to a compatible precision. For example, \(\log(0.4994/0.5006)\approx-0.0024\), not \(-0.0022\); the latter is appropriate only for a probability endpoint closer to \(0.49944\).
Key takeaway: A Wald interval uses one local curvature value and is symmetric around the estimate. A profile interval follows the likelihood-ratio contour across the parameter space, so changing curvature and skewness can make its endpoint distances unequal. The quadratic approximation explains why the two methods can agree near the maximum; higher-order shape explains why they may diverge.

Check Your Understanding

Answer these questions using the definitions and calculations above.

  1. What feature of the Wald construction forces its endpoints to be equally distant from the estimate?
  2. In the two-event example, which profile endpoint is farther from \(\hat\beta\), and by approximately how much?
  3. Why does the local quadratic approximation produce symmetric likelihood-ratio endpoints?
  4. In the cubic expansion, what does the sign of \(\ell_p'''(\hat\beta)\) indicate about the direction of the leading endpoint shift?
  5. Why should an asymmetric profile interval not automatically be described as having exact 95% coverage?
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