The delta method and functional delta method
Propagate weak limits through smooth maps while respecting the tangent space.
On this page
The question for today
What you’ll understand
- Apply a derivative to a vector-valued asymptotic distribution.
- State a tangential Hadamard differentiability condition for a functional.
- Diagnose a vanishing derivative and calculate a quantile limit.
An estimator often becomes useful only after transformation: a probability becomes log odds, a distribution becomes a quantile, or a vector becomes a contrast. The delta method transfers a known weak limit through an appropriate derivative. Its content is a remainder estimate strong enough to remain negligible at the statistical scale. Ordinary derivatives suffice in finite dimensions; functionals of an empirical distribution need a stronger notion that remains stable along converging directions. A zero derivative is a warning that the first-order limit may conceal the relevant fluctuations.
Linearization at the statistical scale
Suppose the root-sample-size error of a vector estimator converges weakly to a tight random vector. If the transformation is differentiable at the true parameter, its linear approximation carries this limit to the derivative applied to that vector. For a normal input limit, the transformed covariance is obtained by multiplying on the left and right by the derivative and its transpose. The covariance formula describes the limiting scaled error; dividing it by sample size gives a large-sample variance approximation.
The derivative is evaluated at the population parameter in the theorem. A practical standard error may substitute a consistent estimator if the derivative and variance formula are continuous nearby. Transformations with singularities require checking that the true parameter lies away from them. For instance, log odds is smooth for an interior probability, but its derivative diverges at zero and one. A formula derived for a fixed interior probability does not automatically remain valid for probabilities approaching a boundary with sample size.
Why a functional needs stable directional derivatives
For a map between normed spaces, Hadamard differentiability tangentially to a set of directions asks that difference quotients converge along every admissible sequence of directions approaching a tangent direction. The derivative must be continuous and linear on the tangent space. If the scaled input error converges weakly to a tight limit supported on that space, the functional delta method applies. All perturbed inputs must remain in the map's domain; arbitrary signed perturbations of a distribution are not automatically distributions.
For a fixed quantile level strictly between zero and one, assume the distribution is differentiable at its unique target quantile with a positive derivative there. The inverse-distribution functional has derivative given below, along directions continuous at the quantile, using the usual uniform topology for distribution perturbations. Empirical-distribution fluctuations converge to a Brownian bridge, whose variance at that location is the level times one minus the level. A process theorem for many quantiles needs stronger uniform density conditions; the single-quantile calculation does not assert those.
When the first derivative vanishes
A zero derivative yields a zero first-order limit rather than a useful normal approximation. Consider squaring an estimator whose true parameter is zero and whose root-sample-size limit is centered normal with variance . Multiplying the squared estimator by sample size then gives a scaled chi-square limit with scale . This follows directly from the continuous mapping theorem applied to the original root-sample-size error. It requires a different normalization from the first-order delta method.
Likewise, the existence of directional derivatives one direction at a time does not establish the functional theorem. The directions themselves fluctuate with the sample, so stability under changing directions matters. Maxima, kinks, and active inequality constraints can have nonlinear directional derivatives and nonnormal limits. They need a suitable directional theory or a direct calculation. Before using an automatic standard-error recipe, identify the input space, topology, limiting process, derivative, and any loss of first-order information.
Work it through
Log odds of a Bernoulli probability
For independent Bernoulli observations with , transform an interior sample proportion by and define the transformed estimate to be zero on sample proportions zero or one. These endpoint events have probabilities tending to zero. Find its first-order asymptotic variance and an approximate standard error at sample size .
The proportion has root-sample-size variance . The probability is interior, so the log-odds derivative exists and equals .
Multiply the original variance by the squared derivative. The resulting root-sample-size variance simplifies to , rather than its square.
Divide by and take a square root: the standard-error approximation is . This uses the population probability to display the calculation; an applied estimate would plug in a consistent interior proportion.
The transformed error is asymptotically normal with variance at root-sample-size scale. This is an asymptotic statement even though the original proportion has an exact finite-sample binomial law.
The living notebook
Explore the model
Interactive lab · function
A derivative can erase the first-order term
Pause/Reset and set BOTH controls to , . Predict and slope . For a fresh comparison Pause/Reset and set BOTH to , : value and slope are zero, although the function still curves upward. Parameter changes pause and retain the clock; Reset clears it.
- y at chosen x
- 0.608
- Tangent slope · 2ax
- 1.35
- Signed area · ax³/3
- 0.182
This lab uses only y = ax². Playback traces the curve within the fixed integration interval from 0 to x; it does not estimate numerical error or change the chosen point. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.
Look forThe quadratic shows why a zero derivative can hide second-order behavior. It does not compute a functional derivative or a sampling distribution.
Pause & reason
Check your understanding
Your turn
Try it yourself
For a uniform distribution on , calculate the derivative and limiting variance of the empirical first quartile. What standard-error approximation results at sample size ?
Take a moment to make a prediction or work it out on paper. Open a hint when you need one.
Give me a hint
Use the density at the first quartile and the Brownian-bridge variance .
Compare with the solution
Here , , and . The derivative sends a direction to . The root-sample-size variance is . Thus the approximate standard error is . The positive interior density justifies the inverse derivative; the compact support endpoints do not interfere at this quantile.
Keep the idea
Take it with you
- Apply the derivative to the limiting random object, with its covariance transformed accordingly.
- Functional differentiability must remain stable along admissible converging directions.
- A vanishing derivative can require a new rate and a nonnormal limit.
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