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Linear Quadratic Control with Non-Markovian and Non-Semimartingale Noise Models

This paper utilizes rough path theory, specifically signature representations and controlled rough paths, to solve a generalized linear quadratic optimal control problem involving non-Markovian and non-semimartingale noise processes with low Hölder regularity.

Original authors: Mostafa M. Shibl, Sharan Srinivasan, Harsha Honnappa, Vijay Gupta

Published 2026-02-11
📖 3 min read☕ Coffee break read

Original authors: Mostafa M. Shibl, Sharan Srinivasan, Harsha Honnappa, Vijay Gupta

Original paper licensed under CC BY 4.0 (http://creativecommons.org/licenses/by/4.0/). This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

Imagine you are trying to teach a self-driving car how to stay in its lane on a highway.

The Old Way: The "Smooth Road" Assumption

Standard engineering math (called LQG control) assumes the world is a bit like a gentle, predictable breeze. It assumes that any "noise"—like wind hitting the car or a bump in the road—follows a very specific pattern called "Brownian motion."

Think of Brownian motion like a series of tiny, random, but relatively "polite" nudges. Because these nudges are predictable in their randomness, engineers have a perfect mathematical playbook to counteract them. If the wind nudges the car left, the math says, "Don't panic, just nudge it right by exactly this much."

The Problem: The "Wild World" Reality

The authors of this paper argue that the real world isn't "polite." Real-world noise is often non-Markovian and non-semimartingale. That sounds like a mouthful, but here is what it actually means:

  1. Non-Markovian (The "Memory" Problem): Standard math assumes the future only depends on where you are now. But real noise has a memory. Imagine driving through a storm where the wind isn't just random; it has a rhythm. If a gust hits you now, it’s highly likely a similar gust will hit you in three seconds. The "noise" has a history.
  2. Non-Semimartingale (The "Jagged" Problem): Standard math assumes the road is mostly smooth. But some real-world noise is incredibly "jagged" and "rough"—like driving over a field of broken glass or through a sudden earthquake. The movements are so sharp and irregular that the old mathematical tools literally break; they can't even calculate the "average" movement because the path is too chaotic.

If you use the "Smooth Road" playbook in a "Broken Glass" world, your self-driving car will overreact, panic, and eventually fly off the road.

The Solution: "Rough Path Theory" (The High-Definition Map)

The researchers introduced a new mathematical framework called Rough Path Theory.

If standard calculus is like looking at a blurry, low-resolution photo of a road, Rough Path Theory is like looking at a high-definition, 3D topographical map.

Instead of just looking at where the car is, this theory looks at the "signature" of the noise. It doesn't just see a nudge; it sees the shape, the rhythm, and the intensity of the turbulence. It uses something called "iterated integrals"—think of this as the math's way of saying, "I'm not just looking at the current bump; I'm calculating how the last five bumps are likely to influence the next one."

The Results: Staying on the Road

To prove this works, they tested it on a digital "Inverted Pendulum" (a classic physics test where you try to balance a stick on your finger).

  • The Old Controller: When they hit the pendulum with "jagged" noise (like a sudden earthquake or a heavy-tailed jump), the old controller panicked. It tried to correct too hard, hit its limit, and the pendulum went flying wildly out of control.
  • The New "gLQ" Controller: The new controller saw the "jaggedness" coming. It used its "memory" and its "high-def map" to make smooth, intelligent corrections. Even when the noise was chaotic and unpredictable, the pendulum stayed perfectly upright.

Summary in a Nutshell

The Paper's Core Message: Most control systems are designed for a "polite" world. This paper provides a new mathematical toolkit for a "wild" world, allowing machines to remain stable and safe even when faced with the most jagged, unpredictable, and "memory-heavy" chaos nature can throw at them.

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