CLT-Optimal Parameter Error Bounds for Linear System Identification
TLDR
This paper provides sharper, instance-optimal parameter error bounds for linear system identification, improving on current state-of-the-art methods.
Key contributions
- Reveals current linear system identification bounds overstate parameter error by state-dimension factor.
- Identifies problem instances where existing bounds are statistically inaccurate.
- Introduces a novel second-order decomposition for sharper parameter error analysis.
- Achieves finite-sample bounds matching instance-specific optimal rates in Frobenius norm.
Why it matters
Current system identification error bounds are statistically inaccurate, overstating errors. This paper provides significantly sharper, instance-optimal bounds. These improved bounds are crucial for accurately evaluating and advancing linear system identification algorithms.
Original Abstract
There has been remarkable progress over the past decade in establishing finite-sample, non-asymptotic bounds on recovering unknown system parameters from observed system behavior. Surprisingly, however, we show that the current state-of-the-art bounds do not accurately capture the statistical complexity of system identification, even in the most fundamental setting of estimating a discrete-time linear dynamical system (LDS) via ordinary least-squares regression (OLS). Specifically, we utilize asymptotic normality to identify classes of problem instances for which current bounds overstate the squared parameter error, in both spectral and Frobenius norm, by a factor of the state-dimension of the system. Informed by this discrepancy, we then sharpen the OLS parameter error bounds via a novel second-order decomposition of the parameter error, where crucially the lower-order term is a matrix-valued martingale that we show correctly captures the CLT scaling. From our analysis we obtain finite-sample bounds for both (i) stable systems and (ii) the many-trajectories setting that match the instance-specific optimal rates up to constant factors in Frobenius norm, and polylogarithmic state-dimension factors in spectral norm.
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