On the Equivalence of Stochastic Control and Path Space Formulations for Schrödinger Bridges over Compact Connected Lie Groups
Hamza Mahmood, Georgiy A. Bondar, Abhishek Halder, Adeel Akhtar
math.OC · cs.AI · eess.SY · math.PR · stat.ML
Quick verdict
Proves control-vs-path-space (relative entropy) equivalence for Schrödinger bridges on compact Lie groups via Girsanov; sound but validation is qualitative.
Summary
This paper proves that, for stochastic kinematics on a compact connected Lie group, the Schrödinger bridge problem (SBP) posed as stochastic optimal control is equivalent to minimizing relative entropy over path measures with prescribed endpoint marginals. The route is intrinsic: a horizontal lift and stochastic anti-development express the group-valued controlled diffusion in Euclidean coordinates, yielding a Girsanov change of measure (Lemma 1) even though tangent spaces vary along trajectories — extending a Euclidean result ([9, Thm 4.2]) beyond the matrix-Lie-group framework of Karandikar. Corollary 1 shows the expected control energy equals 1/(2σ²) times the KL divergence of the controlled path law against the reference Wiener measure. Three implications follow: a direct existence-uniqueness proof (Theorem 1) via weak compactness and an h-transform exactness argument, complementing the authors' earlier Schrödinger-system route; a Sanov large-deviation reading of the bridge as the most probable path-law deviation; and computation of the optimal path measure by static Sinkhorn recursions on endpoint samples. Limitations: the equivalence formally requires every admissible control to satisfy progressive measurability, well-posedness in law and a Novikov exponential-moment condition — finite energy alone guarantees none of these — and the numerical illustration on T² is qualitative only (50 endpoint samples, no error metric, unreported diffusion strength). Code is public.
Review complete
Assessment at a glance
4
risk flags identified
● high 0
● medium 2
● low 2
4 strengths · 5 weaknesses · 5 author questions
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Key claims under review
- Under progressive measurability, well-posedness in law and Novikov conditions, the stochastic exponential (14) defines a Girsanov change of measure on C([0,1];G) that turns the canonical diffusion into the controlled SDE (12) (Lemma 1).
- The expected control energy equals (1/2σ²) times the KL divergence of the controlled path law from the reference Wiener measure (Corollary 1, eq. 25).
- Consequently the SBP on G is equivalent to minimizing relative entropy over path measures with prescribed endpoint marginals, and this problem admits a unique minimizer that solves Problem 1 (Theorem 1).
- By Sanov's principle, the optimal bridge is the most probable path-measure deviation of the uncontrolled dynamics consistent with the endpoint constraints.
- Static Sinkhorn recursions on endpoint samples compute the optimal path measure, matching the dynamic PDE-based solution in the T² example.
Strengths
Intrinsic Girsanov construction on Lie groups
Lemma 1 handles the key difficulty — driving noise living in tangent spaces that vary along trajectories — via horizontal lift and stochastic anti-development (eqs. 9-11, 14-16), rather than the logarithm/exponential map route that restricts Karandikar's 1983 result [11] to matrix Lie groups.
Exact and correctly proven energy-entropy identity
Corollary 1 (eq. 25) derives DKL(PΩ‖W)= (1/2σ²)·E[∫‖Ω‖²dt] via the standard martingale argument, with the finite-energy condition (24) imposed exactly where the martingale expectation needs it; the orthogonality step via Ot (eq. 23) is clean.
Direct existence-uniqueness proof honestly contrasted with prior work
Actionable computational payoff with public code
Weaknesses
Admissible class gap between V and Assumptions 1-3
Relaxation-exactness step delegated to citation
Numerical evidence is qualitative only
Incremental novelty over known Euclidean theory
Large-deviation section is informal
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Scope & Claims
The paper (arXiv 2609.13758, control-letter format, math.OC-flagged) makes three claims for the Schrödinger bridge problem (SBP) on a compact connected Lie group G. First, a Girsanov-type change of measure between the reference Wiener measure of (8) and the law of the controlled Stratonovich SDE (12), obtained intrinsically via horizontal lift and stochastic anti-development (Lemma 1, eqs. 14-16). Second, the exact identity between expected control energy and path-space relative entropy, DKL = (1/2σ²)·E[∫‖Ω‖²dt] (Corollary 1, eq. 25). Third, three consequences: a direct existence-uniqueness proof (Theorem 1), a Sanov large-deviation reading of the bridge as the most probable path-law deviation (Sec. III.A), and a static Sinkhorn route to the optimal path measure, illustrated on T² (Sec. IV). The Euclidean analogue is acknowledged upfront ([9, Thm 4.2]); the contribution is the intrinsic Lie-group extension beyond Karandikar's matrix-Lie-group framework [11], where the noise lives in a fixed Lie algebra rather than trajectory-varying tangent spaces.
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Frequently asked questions
What is the main result of this paper?
It proves that on a compact connected Lie group, solving the Schrödinger bridge problem as a stochastic optimal control problem is mathematically equivalent to minimizing relative entropy (KL divergence) over path measures with fixed endpoint distributions: the expected control energy equals 1/(2σ²) times that KL divergence. This generalizes a known Euclidean-space equivalence to Lie groups, where the noise lives in tangent spaces that vary along each trajectory.
How does it differ from previous Schrödinger bridge work?
Earlier path-space equivalence results held on Euclidean state spaces or, for Lie groups, only for matrix Lie groups via logarithm/exponential maps. This paper uses a horizontal lift and stochastic anti-development to handle any compact connected Lie group intrinsically, and it also gives a direct existence-uniqueness proof complementing the same authors' earlier paper that solved the Lie-group SBP via the Schrödinger system of PDEs.
Is code available for this paper?
Yes. The repository is github.com/gradslab/LargeDeviationSBP, with additional simulations and animations hosted at gradslab.github.io/LargeDeviationSBP. The numerical example compares a dynamic Sinkhorn PDE solve on a 128×128 torus grid with a static Sinkhorn solve on 50 sampled endpoint points.
What does 'most probable deviation' mean in this context?
By Sanov's large-deviation principle, the probability that empirical paths of the uncontrolled dynamics concentrate near a given path measure decays exponentially at rate equal to its KL divergence from the reference Wiener measure. Among all path measures matching the prescribed endpoint marginals, the Schrödinger bridge minimizes that rate, so it is the least unlikely — most probable — way the free dynamics could deviate while respecting the endpoint constraints.
About this review
This is an AI-generated preliminary review by Evolve.Pub, produced from the openly available text of the paper. It is not peer review and does not represent the authors' views. The canonical record of the paper is at the publisher link above.
- Figure 1 is an image; only its caption was extractable, so the claimed visual agreement between the two solutions could not be independently inspected.
- Inline math and equation numbering are mangled in places by PDF extraction (standard artifact); proofs were read with that in mind, and the reference list ends completely with [18], so no truncation is suspected.
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