This paper introduces the HARQ family of realized-volatility forecasting models, which improve on the standard HAR model by letting the autoregressive parameters vary explicitly with the amount of measurement error in the realized-volatility (RV) regressor. Realized volatility equals the true latent integrated volatility (IV) plus a serially uncorrelated measurement error, so forecasting IV from observed RV is a classical errors-in-variables problem that attenuates the persistence parameter. Because high-frequency asymptotic theory says the size of that error is governed by integrated quarticity — consistently estimable by realized quarticity (RQ) — the models can adapt: when today's RV is precisely measured (low RQ), the model weights it more, producing stronger persistence and more responsive forecasts; when RV is noisy, it shrinks the weight. Applied to the S&P 500 and Dow constituents, HARQ delivers substantial out-of-sample forecast gains over HAR and other standard models.
"By allowing the parameters of the models to vary explicitly with the (estimated) degree of measurement error, the models exhibit stronger persistence, and in turn generate more responsive forecasts, when the measurement error is relatively low."
The move here is elegant because it turns a nuisance — the estimation error in realized volatility — into a usable signal. Everyone knew RV was a noisy proxy for IV; the insight is that high-frequency theory tells you how noisy on each specific day (via realized quarticity), so you can down-weight the days you should distrust rather than applying one fixed, attenuated coefficient. That it stays a plain OLS regression is what made HARQ catch on as a default upgrade to Corsi's HAR. It complements the wiki's realized-volatility and Andersen-Bollerslev material by taking the measurement-error problem those pages raise and building the correction directly into the forecasting equation. The main caveats are practical: realized quarticity is itself noisily estimated (a fourth moment), so the correction can be jumpy, and the linear form is a convenient approximation rather than the exact optimal weight.