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A unified theory of order flow, market impact, and volatility

Johannes Muhle-Karbe, Youssef Ouazzani Chahd, Mathieu Rosenbaum, Grégoire Szymanski

TL;DR

The paper develops a unified microstructural model for order flow by separating core and reaction components as Hawkes processes. In a scaling-limit regime, a single persistence parameter $H_0$ governs the behavior of signed order flow, unsigned volume, volatility, and the market impact function, linking long-range memory with rough dynamics and a power-law impact $MI(t) \sim t^{2-2H_0}$. Empirically, $H_0$ is estimated around $0.75$--$0.8$, which simultaneously reproduces persistent order flow, rough volume near $H_0-1/2$, and very rough volatility with $2H_0-3/2$, while recovering the square-root market impact at $H_0=3/4$. The framework provides a principled explanation for the joint scaling properties of microstructure and price dynamics and positions markets at the edge of criticality, where prices stay diffusive yet volatility remains ultra-rough.

Abstract

We propose a microstructural model for the order flow in financial markets that distinguishes between {\it core orders} and {\it reaction flow}, both modeled as Hawkes processes. This model has a natural scaling limit that reconciles a number of salient empirical properties: persistent signed order flow, rough trading volume and volatility, and power-law market impact. In our framework, all these quantities are pinned down by a single statistic $H_0$, which measures the persistence of the core flow. Specifically, the signed flow converges to the sum of a fractional process with Hurst index $H_0$ and a martingale, while the limiting traded volume is a rough process with Hurst index $H_0-1/2$. No-arbitrage constraints imply that volatility is rough, with Hurst parameter $2H_0-3/2$, and that the price impact of trades follows a power law with exponent $2-2H_0$. The analysis of signed order flow data yields an estimate $H_0 \approx 3/4$. This is not only consistent with the square-root law of market impact, but also turns out to match estimates for the roughness of traded volumes and volatilities remarkably well.

A unified theory of order flow, market impact, and volatility

TL;DR

The paper develops a unified microstructural model for order flow by separating core and reaction components as Hawkes processes. In a scaling-limit regime, a single persistence parameter governs the behavior of signed order flow, unsigned volume, volatility, and the market impact function, linking long-range memory with rough dynamics and a power-law impact . Empirically, is estimated around --, which simultaneously reproduces persistent order flow, rough volume near , and very rough volatility with , while recovering the square-root market impact at . The framework provides a principled explanation for the joint scaling properties of microstructure and price dynamics and positions markets at the edge of criticality, where prices stay diffusive yet volatility remains ultra-rough.

Abstract

We propose a microstructural model for the order flow in financial markets that distinguishes between {\it core orders} and {\it reaction flow}, both modeled as Hawkes processes. This model has a natural scaling limit that reconciles a number of salient empirical properties: persistent signed order flow, rough trading volume and volatility, and power-law market impact. In our framework, all these quantities are pinned down by a single statistic , which measures the persistence of the core flow. Specifically, the signed flow converges to the sum of a fractional process with Hurst index and a martingale, while the limiting traded volume is a rough process with Hurst index . No-arbitrage constraints imply that volatility is rough, with Hurst parameter , and that the price impact of trades follows a power law with exponent . The analysis of signed order flow data yields an estimate . This is not only consistent with the square-root law of market impact, but also turns out to match estimates for the roughness of traded volumes and volatilities remarkably well.
Paper Structure (21 sections, 11 theorems, 156 equations, 5 figures, 1 table)

This paper contains 21 sections, 11 theorems, 156 equations, 5 figures, 1 table.

Key Result

Theorem 3.1

Under Assumptions assumption:jaisson:long_memory:1 and assumption:jaisson:long_memory:2, the process $(\overline F_{t}^{+, T}, \overline F_{t}^{-, T})_{t \in [0,1]}$ is tight for the Skorokhod topology. Furthermore, any limit point $(F_{t}^{+}, F_{t}^{-})$From now on $(F_{t}^{+}, F_{t}^{-})$ denote where $Z^{+}$ and $Z^-$ are two independent continuous martingales with quadratic variations $F^{+}

Figures (5)

  • Figure 1: Cumulative signed order flow of the representative stock LVMH between 2021 and 2024.
  • Figure 2: Daily traded volume of the representative stock LVMH between 2021 and 2024.
  • Figure 3: Average Hurst exponent estimates for signed order flow over 40 stocks for the period 2021--2024, under fractional Brownian motion specification. Note: The data used for the estimations throughout the paper are described in Appendix \ref{['app:data']}.
  • Figure 4: Average Hurst exponent estimates for signed order flow over $40$ stocks for the period 2021--2024, under mixed fractional Brownian motion specification. Note: For each asset and time scale $\Delta$, the Hurst parameter of the fractional Brownian motion component is estimated using quadratic variations computed at the time scales $\Delta$, $2\Delta$, and $4\Delta$. The estimation procedure then follows the methodology developed for mixed fractional processes in CDM22szymanski2026mixed.
  • Figure 5: Average Hurst exponent estimates for unsigned trading volume, averaged over $40$ stocks for the period 2021--2024. Note: For each asset and time scale $\Delta$, the procedure is as follows: the total traded volume is aggregated over bins of size $\Delta$; the intraday seasonal pattern is removed multiplicatively; volume increments are computed and truncated at three times their standard deviation to mitigate the impact of outliers and exclude potential jumps in the volume intensity process; the auto-covariance function is then estimated, and the Hurst exponent is obtained using a GMM-based approach similar to li2016generalized. The methodology closely follows the procedures developed for volatility analysis in chong2022CLTchong2026intraday.

Theorems & Definitions (15)

  • Theorem 3.1
  • Proposition 3.2
  • Proposition 3.3
  • Theorem 3.4
  • Theorem 3.5
  • Theorem 3.6
  • Theorem 4.1
  • Remark 4.2
  • Definition A.1
  • Lemma A.2
  • ...and 5 more