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The Canonical Joint Distribution · Tutorial 47 of 699

Why Score Increments Are Asymptotically Independent

See how regular likelihood scores and information increments yield asymptotically independent standardized block scores, and learn when that approximation may fail.

Advanced 12 min read

What You'll Learn

  • Define a score increment and its corresponding Fisher information increment.
  • State the regularity and large-block conditions for asymptotic normality.
  • Derive joint asymptotic independence from block independence and a central limit theorem.
  • Extend the justification to martingale score increments with deterministic limiting information.
  • Standardize efficient score increments when a regular nuisance parameter is present.
  • Recognize why zero covariance or a small information block alone does not justify the approximation.

Why Score Increments Become Independent

At successive analyses, the data collected since the previous analysis contribute a new score increment. In a regular model, that increment has mean zero under the null and variance described by the information accumulated in that block. When blocks contain enough information, standardized increments are approximately normal. If the blocks are independent, their joint approximation is a collection of independent normal variables.

The distinction between independence and asymptotic normality matters. With independent observations assigned to fixed, nonoverlapping blocks, the block scores are already independent at finite sample sizes. What is usually asymptotic is their normal approximation. In sequential settings where increments need not be exactly independent, a martingale central limit argument can give asymptotically independent Gaussian increments under suitable conditions.

Definition: Let \(\theta\) be a scalar parameter, and let \(s_i(\theta_0)\) be the score contribution from observation \(i\), evaluated at the null value \(\theta_0\). For a block \(B_k\) of observations, its score increment and information increment are $$ \Delta U_k=\sum_{i\in B_k}s_i(\theta_0), \qquad \Delta I_k=\sum_{i\in B_k} I_i(\theta_0), $$ where \(I_i(\theta_0)=E_{\theta_0}\{s_i(\theta_0)^2\}\) is the Fisher information contribution. The standardized score increment is \(Z_k=\Delta U_k/\sqrt{\Delta I_k}\), when \(\Delta I_k>0\).

The usual regularity conditions ensure that each score has mean zero and that its variance agrees with the expected negative second derivative of the log likelihood. For independent observations, disjoint blocks then have independent score increments. The central limit theorem supplies the approximate normal distribution when each block's information grows and no individual observation dominates that block.

For a fixed number of blocks, a useful version of the conditions is that the observations are independent, the expected information in each block tends to infinity, and a Lindeberg condition holds within each block. In words, the condition rules out a material share of the block's score variation coming from rare, exceptionally large contributions. The model must also be identifiable and differentiable near \(\theta_0\), with finite, positive information. These conditions are not automatic merely because a score can be calculated.

Derivation for Independent Blocks

Under \(H_0\), regularity gives \(E_{\theta_0}\{s_i(\theta_0)\}=0\). If observations are independent, scores from different observations are independent. Consequently, score increments formed from disjoint blocks are independent, and $$ E_{\theta_0}(\Delta U_k)=0, \qquad \operatorname{Var}_{\theta_0}(\Delta U_k)=\Delta I_k. $$ The central limit theorem, applied separately to each block, gives \(Z_k\) an approximate standard normal distribution. Independence of the blocks makes the joint characteristic function factor into the product of the block characteristic functions. Since each factor converges to the characteristic function of a standard normal variable, the joint limit is a vector of independent standard normal variables.

$$ E_{\theta_0}\!\left[\exp\!\left(i\sum_{k=1}^K t_k Z_k\right)\right] =\prod_{k=1}^K E_{\theta_0}\{\exp(it_kZ_k)\} \ \longrightarrow\ \prod_{k=1}^K \exp(-t_k^2/2). $$

The right-hand side is the joint characteristic function of independent \(N(0,1)\) variables. Thus, for a fixed number \(K\) of blocks, the standardized score increments converge jointly to independent standard normal variables. This argument uses more than zero covariance: it uses independence of the blocks at finite sample sizes, followed by a normal limit for each block.

There is another route when observations arrive sequentially and score increments are martingale differences rather than independent variables. A martingale difference has conditional mean zero given the past. If its accumulated conditional variance, after standardization, converges to a nonrandom value, and a martingale Lindeberg condition prevents large contributions, a martingale central limit theorem yields a Gaussian limit. For several consecutive blocks, the same argument applied jointly gives a Gaussian vector whose components have zero cross-covariances when the limiting information increments are nonoverlapping. In a Gaussian vector, zero cross-covariance implies independence. This is asymptotic independence; the original increments need not be independent.

Worked Example: Two Independent Blocks in an IID Regular Model

Suppose a hypothetical regular model has independent, identically distributed observations and Fisher information \(I_i(\theta_0)=2.5\) per observation. The first block contains 80 observations and the second contains 120. Assume the score contributions have finite variance and satisfy the usual central limit theorem conditions.

The information increments are $$ \Delta I_1=80(2.5)=200, \qquad \Delta I_2=120(2.5)=300. $$ Suppose the observed score increments are \(\Delta U_1=12\) and \(\Delta U_2=-8\). Their standardized values are $$ Z_1=\frac{12}{\sqrt{200}}=0.8485, \qquad Z_2=\frac{-8}{\sqrt{300}}=-0.4619. $$

Because the blocks contain disjoint independent observations, the two raw score increments are independent in this model; dividing each by its fixed information-based scale preserves that independence. With sufficiently large blocks, their joint distribution is approximated by that of two independent standard normal variables under \(H_0\). The displayed values are observed statistics, not evidence that the assumed distribution or independence conditions hold.

Heterogeneous Information and Sequential Scores

Equal block sizes are not required. If observations are independent but have different information contributions, the variance of a block score is the sum of those contributions. Standardizing by the block's own \(\Delta I_k\), rather than by its number of observations, is what puts increments on a common scale. The large-block requirement concerns information and the distribution of score contributions, not just a raw count.

Worked Example: Unequal Information Across Blocks

Consider a hypothetical sequence of independent, non-identically distributed observations. Suppose the first block has total information \(\Delta I_1=90\), the second has \(\Delta I_2=160\), and their observed score increments are 9 and \(-12\). Assume, for the sequence of models being considered, that each block's information grows and its score contributions satisfy the Lindeberg condition.

The appropriate standardizations are $$ Z_1=\frac{9}{\sqrt{90}}=0.9487, \qquad Z_2=\frac{-12}{\sqrt{160}}=-0.9487. $$

The independent observations make the two block scores independent. Under the stated large-block conditions, the standardized pair is approximately distributed as independent standard normals under \(H_0\). Unequal information totals do not prevent this conclusion: each increment is divided by its own standard deviation. The numbers alone, however, cannot verify the Lindeberg condition; that condition concerns the score-contribution distributions, not just the totals.

The same reasoning applies to an efficient score when a regular nuisance parameter is present. For a scalar target parameter \(\psi\) and scalar nuisance parameter \(\lambda\), let the information matrix for one observation at the null be $$ I= \begin{pmatrix} I_{\psi\psi} & I_{\psi\lambda}\\ I_{\lambda\psi} & I_{\lambda\lambda} \end{pmatrix}. $$ If \(I_{\lambda\lambda}>0\), the efficient score contribution for \(\psi\) is \(s_{\psi,i}-(I_{\psi\lambda}/I_{\lambda\lambda})s_{\lambda,i}\). Its variance is the efficient information \(I_{\psi\psi}-I_{\psi\lambda}^2/I_{\lambda\lambda}\). Using that score and its information in each block preserves the block argument when the nuisance parameter is handled under the same regular model.

Worked Example: Efficient Score Increments With a Nuisance Parameter

Suppose a hypothetical two-parameter regular model has per-observation information $$ I= \begin{pmatrix} 4 & 1\\ 1 & 2 \end{pmatrix}, $$ where \(\psi\) is the target and \(\lambda\) is a nuisance parameter. The efficient score contribution for \(\psi\) is \(s_{\psi,i}-\tfrac12s_{\lambda,i}\), because \(I_{\psi\lambda}/I_{\lambda\lambda}=1/2\). Its information per observation is $$ I_{\mathrm{eff}}=4-\frac{1^2}{2}=3.5. $$

Let two independent blocks contain 50 and 70 observations. Their efficient information increments are \(50(3.5)=175\) and \(70(3.5)=245\). Suppose the sums of efficient scores in the blocks are 7 and \(-14\). Then $$ Z_1=\frac{7}{\sqrt{175}}=0.5292, \qquad Z_2=\frac{-14}{\sqrt{245}}=-0.8944. $$

Provided the model is regular, the information matrix is nonsingular, and the blocks satisfy the large-sample conditions, these standardized efficient score increments are approximately independent standard normal variables under \(H_0\). The nuisance adjustment is part of defining the score increment; it does not remove the need to check regularity and block conditions.

Diagnostics, Alternatives, and Limits

The independent-increment approximation is most credible when the data are collected in fixed, nonoverlapping blocks from an independent-observation model, or when a suitable martingale formulation applies. Check that the score is evaluated under the stated null model, the information is positive and correctly calculated, every block has enough information for its normal approximation, and no single observation or cluster dominates. If the data are dependent, or if a block boundary is selected using earlier outcomes, ordinary independence of block scores cannot simply be assumed. A sequential model and its conditional information structure must justify the alternative argument.

A common mistake is to argue, “The score increments have zero covariance, so they are independent.” Zero covariance alone does not establish independence for general, nonnormal variables. The correction is to justify independence from independent data blocks, or to establish a joint Gaussian limit and then use the fact that uncorrelated components of a Gaussian vector are independent. A related mistake is to call the increments asymptotically independent without checking that each block has enough information for the required limit.

Two useful approaches answer related but different questions. A direct covariance calculation identifies covariance under a specified model, but zero covariance alone may not settle independence. The score-process approach explains why a joint Gaussian approximation can arise and when its increments are independent. Alternatively, a canonical joint normal model specifies the joint distribution directly; the score argument provides a regular-model justification for that kind of approximation rather than replacing its assumptions with a universal guarantee.

The conclusion is limited to the model and asymptotic regime used in the argument. Small or sparse blocks, heavy-tailed score contributions, non-identifiability, boundary parameter values, or misspecified information can invalidate the normal approximation. Shared nuisance-parameter estimates or data-dependent changes to the analysis can also complicate the block structure. In these cases, the issue is not fixed merely by dividing each score by the square root of an information estimate.

Key takeaway: Disjoint independent blocks give independent score increments exactly, while regularity and a blockwise central limit theorem make their standardized values approximately normal. In sequential settings without exact independence, martingale conditions can yield asymptotic independence through a joint Gaussian limit. The data structure, information, and large-block conditions must support the chosen argument.

Check Your Understanding

Answer each question using the stated model conditions. Short solutions follow the questions.

  1. Under what two distinct facts do independent-block standardized scores have an approximate joint distribution of independent standard normals?
  2. Two disjoint blocks have independent score increments with information totals 64 and 144. Their observed score increments are 4 and \(-9\). Calculate the standardized increments.
  3. Why does zero covariance between two nonnormal score increments not, by itself, prove independence?
  4. In a martingale score argument, what role does a deterministic limiting conditional variance play?
  5. Does standardizing a score increment by its information guarantee a reliable normal approximation when the block has very little information? Explain.

Solutions. (1) Independent blocks establish independence of their increments, and a central limit theorem for each sufficiently informative block supplies the approximate standard normal distributions. (2) \(4/\sqrt{64}=0.5000\) and \(-9/\sqrt{144}=-0.7500\). (3) Uncorrelated variables can still be dependent unless additional structure, such as joint normality, is established. (4) Together with the martingale conditions, it gives the Gaussian limit's variance structure; disjoint limiting increments then have zero cross-covariance and are independent in that Gaussian limit. (5) No. Standardization sets a scale but does not ensure that the score's distribution is close to normal; block size, information, and the score-contribution conditions still matter.

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