The term structure of the flow skew
The finite-horizon behavior of the imbalance equivalence. Companion to On a Simple Relationship Between Order Imbalance, Skew and Width in Over-The-Counter Trading; a note on the finite-horizon case is in preparation.
The steady-state theory says one-sided flow displaces a dealer's quoted mid by the constant $\delta = \tfrac{1}{2k}\log(A^b/A^a)$. At finite horizon that is not what happens. In the model of Guéant, Lehalle and Fernandez-Tapia with asymmetric arrival scales, the problem is exactly conjugate to a balanced one, but the imbalance lands in the terminal condition: the dealer's flow is balanced around the shifted price $S - \delta$ while her book is marked at $S$. That mismatch makes the flow displacement a term structure: zero at maturity, converging to $-\delta$ at the spectral-gap rate as the horizon grows.
Look for: the displacement curve leaving zero at maturity and climbing to the dashed $-\delta$ line at the spectral rate; the spread's finite-horizon transient; and the violet line — a dealer who marks her terminal book at the flow-adjusted price $S - \delta$ — flat at $-\delta$ for every horizon. One accounting convention turns the term structure back into the constant.
Engine: the paper's exact spectral representation, computed in your browser (fh_core.js): one symmetric eigendecomposition serves every horizon and both markings. Model of Guéant, Lehalle and Fernandez-Tapia (2012) with asymmetric scales; $\sigma = \sqrt{2}$, $k = 1$.