REVIEW 3 major objections 4 minor 2 cited by
Expected Return Symmetries
T0 review · 3 major / 4 minor · reviewed 2026-08-09 · deepseek-v4-flash
Pith's one-line read The paper defines expected return symmetries—transformations preserving optimal-policy returns—and shows they can be learned and used to improve zero-shot coordination beyond environment symmetries.
desk verdict A genuinely new symmetry class for ZSC with strong empirical results, but the theoretical guarantee doesn't cover the policies that OPΦER actually produces. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the expected return symmetry group $\Phi_{\mathrm{ER}}$, the set of transformations of actions and observations that carry every self-play-optimal Boltzmann-exploratory policy to another such policy. Boltzmann-exploratory policies here are softmax policies over local action values at temperature $\alpha$, a choice that ensures suboptimal actions are distinguished by their quality rather than lumped together. The argument runs through the other-play objective $\mathrm{OP}_\Phi(\pi) = \mathbb{E}_{\tilde\pi \in [\pi]}[\mathrm{XP}(\pi, \tilde\pi)]$, where $[\pi]$ is the equivalence class under $\Phi$; using $\Phi_{\mathrm{ER}}$ makes this objective average over diverse optimal conventions. The discovery machinery is gradient-based: with a fixed pool $\Pi'$ of approximately optimal policies, the paper learns $\phi_\theta$ by maximizing $J(\phi_\theta(\pi))$ (Equation 9) or cross-play between policy pairs (Equation 11), searching over action transpositions and a learned observation network, and Equation 10 adds penalties that push the learned maps toward compositionality and invertibility.
What would settle it
Train a held-out set of self-play-optimal Boltzmann-exploratory policies and apply the learned transformations to them: if the expected return of $\phi(\pi)$ is systematically below $J(\pi)$, or if replacing the learned transformations with random policy permutations matched for diversity gives the same cross-play improvement, then the transformations are not expected return symmetries and the coordination gain is not due to the group.
Extended reading notes
Core claim
The central claim is that the right symmetry group for zero-shot coordination is not the group of relabelings that leave the environment dynamics and rewards invariant, but the larger group $\Phi_{\mathrm{ER}}$ of transformations that preserve expected return on the set $\Pi^\alpha_*$ of self-play-optimal Boltzmann-exploratory policies. Formally, $\Phi_{\mathrm{ER}} = \{\phi \in \Psi : \phi(\pi) \in \Pi^\alpha_* \text{ for all } \pi \in \Pi^\alpha_*\}$, which the paper proves is a group under composition and contains the Dec-POMDP symmetries $\Phi_{\mathrm{MDP}}$ as a subgroup. Because $\Phi_{\mathrm{ER}}$ puts more, and more diverse, optimal policies into the same equivalence class, other-play over $\Phi_{\mathrm{ER}}$ trains each agent to be compatible with partners that share its optimality but break conventions differently, which is exactly the failure mode of mutually incompatible symmetry breaking. The paper further claims that approximate elements of $\Phi_{\mathrm{ER}}$ can be learned from interaction alone by maximizing the expected return of transformed fixed optimal policies, with regularization toward compositionality and invertibility, and that this learned group is what delivers the improved zero-shot coordination in the experiments.
Load-bearing premise
The method assumes the transformations trained on a finite pool of good policies really are symmetries of the whole set of optimal policies, and that the approximate invertibility penalty makes them true bijections; if either fails, the group-theoretic coordination guarantees lapse.
Editorial extensions
If this is right
- Other-play with a symmetry group that preserves optimal policies, rather than environment structure, generalizes beyond label relabelings, so independently trained agents can coordinate on any of several equivalent but differently broken optimal conventions.
- Because $\Phi_{\mathrm{MDP}} \subseteq \Phi_{\mathrm{ER}}$, all previous gains from environment-symmetry training are retained, and additional gains appear in games with no non-trivial Dec-POMDP symmetries, such as the cat/dog game.
- Symmetry-based coordination no longer requires privileged knowledge of the environment's transition, reward, or symmetry structure; a model-free agent can discover approximate expected return symmetries from its own interactions.
- A small set of learned transformations can be enough: in Hanabi, 11 learned expected return symmetries produced a within-population cross-play score of 21.64, versus 8.61 for agents using all 120 Dec-POMDP symmetries, while self-play scores stayed near 23.7–24.0.
- The approach works in settings where off-belief learning and cognitive-hierarchy methods fail, including the iterated lever game, the cat/dog game, and Overcooked V2.
Reading between the lines
- If outcome-based symmetry is the right abstraction, the same recipe could be carried to single-agent reinforcement learning: transformations that preserve optimal value would justify data augmentation without knowing the dynamics, and one could test whether policy-space symmetrization improves generalization to unseen tasks.
- The paper fixes action transformations to transpositions and learns observation transformations; a natural extension is to learn joint transformations over continuous or structured action and observation spaces, where bijections are harder, and to check whether the cross-play gains persist.
- A direct test of the mechanism would compare other-play under learned expected return symmetries against other-play under an equal number of random transformations chosen for the same policy diversity; if the random baseline matches the cross-play gains, the gains come from diversity rather than from the group structure.
- The regularized learning objective enforces invertibility only softly, so a stricter parameterization with exact bijectivity could turn the approximate group-theoretic guarantees into quantitative bounds on cross-play degradation.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces expected return symmetries (ΦER), defined as the transformations in Ψ that preserve the set of self-play-optimal Boltzmann-exploratory policies, and argues that this group contains Dec-POMDP symmetries as a subgroup. The authors propose three practical objectives and associated algorithms for learning approximate ER symmetries from agent-environment interaction, and evaluate the resulting other-play variants in four environments. They report that agents trained with OP over learned ER symmetries achieve substantially better zero-shot coordination than self-play or OP over Dec-POMDP symmetries, e.g., Hanabi cross-play of 21.64 versus 8.61 for OP with ΦMDP. The central claims are that ΦER is a broader and learnable symmetry class and that it improves ZSC without privileged environment information.
Significance. If the central claims hold, the paper makes a useful contribution: it identifies a broader symmetry class than Dec-POMDP symmetries, gives a model-free discovery procedure, and provides evidence of practical ZSC gains in several environments. The group-theoretic lemmas in Appendix B are clean, and the main experiments evaluate learned transformations on independently retrained other-play policies, so the reported cross-play improvements are not merely an artifact of the symmetry-fitting procedure itself. The strengths of the paper are its clear formal setup, the substantial empirical gains, and the reproducible code links for several environments. The main weaknesses are that the formal guarantees do not apply to the policies actually produced by the OPΦER learning rule, and that the learned transformations are not certified to be group elements.
major comments (3)
- [§3.2 (Definition 4) and §3.1 (Eq. 7)] Definition 4 constrains transformations only on the set Πα* of self-play-optimal Boltzmann-exploratory policies, but the OP objective in Eq. (4) is maximized over the full policy space Π, and OPΦER-optimal policies are generally not in Πα*. The cat/dog example makes this explicit: the OPΦER-optimal policy is the grounded policy, which is deliberately suboptimal in self-play. For such π ∉ Πα*, the definition of ΦER imposes no constraint on φ(π), so the invariance proofs in Appendix B do not apply to the policies selected by OPΦER. Consequently, the derivation leading to Eq. (7), and the claim that satisfying Items 1 and 2 makes OPΦ equal to expected XP among OPΦ-optimal policies, is incomplete: it requires [π] = ΠΦ* for π ∈ ΠΦ*, which is not established. The empirical check in §4.4, OPΦER(φ(π)) ≈ OPΦER(π), only shows that the orbit of π under the learned transformations has similar OP values; it does not show that the equivalence class of an OPΦER-optimal policy coincides with the set of all OPΦER-optimal policies. This is load-bearing because the theoretical link between the ER-symmetry group and zero-shot coordination depends on it.
- [§3.3 (Eq. 10) and Appendix D] The learned observation transformations are not shown to be bijections on O, or even maps from O to O. In Eq. (10), the invertibility term E_o d(o, φ_θ^2(o))^2 is computed over a continuous extension of O, and the text notes that this extension is needed to avoid a locally constant gradient. The parameterization is a feed-forward neural network with ReLU output in the large-scale experiments, so after training there is no guarantee that φ_O,θ is invertible or that it maps observations to observations. Since membership in ΦER requires an element of Ψ, which consists of bijective maps on S, A, and O, the learned transformations are not certified to lie in ΦER. The group-theoretic guarantees of Appendix B therefore do not apply to the symmetries used in the OP objective. Appendix D gives approximate checks of compositionality and invertibility, but these are measured on a finite set of unseen policies and do not provide a certificate for the actual training procedure.
- [§4.4, Eq. (9), and Algorithms 1–3] The learned symmetries are selected by maximizing expected return on a finite pool Π′ of approximately optimal policies, e.g., k = 6 self-play seeds in Hanabi. This creates a selection bias: a transformation that happens to preserve returns on Π′ may not preserve returns on other self-play-optimal policies or on the policies encountered by OP. The paper acknowledges that the broader Π′ is, the more representative it is, but it does not provide any bound or statistical test connecting the finite-pool objective to preservation on Πα*. The practical claim that the method 'learns' ΦER is therefore only an approximation, and the experimental gains could partly come from generic policy diversity rather than from membership in ΦER. This concern is not fatal to the empirical results, but it should be stated more carefully as an approximation with no formal guarantee.
minor comments (4)
- [§2.3, Eq. (3)] The observation invariance condition contains a typographical error: 'U(ϕ(o_{t+1}) |, ϕ(s_{t+1}), ϕ(a_t))' has an extra comma after the conditioning bar.
- [§3.3, Eqs. (8)–(9)] The text calls Eq. (9) an 'equivalent objective' to Eq. (8), but this equivalence holds only approximately because the policies in Π′ are approximately self-play-optimal; the paper should state this as an approximation rather than an equivalence.
- [§3.3, Algorithms 1 and 2] The pseudocode in Algorithms 1 and 2 loops over all tuples of local action transpositions, but the Hanabi experiments randomly sample 64 transpositions; the algorithms should indicate that random subsampling is part of the described procedure.
- [§4.4, Symmetrizer definition] The symmetrizer S is defined in the experiment section but not in the background; since it plays a role in the reported cross-play results, a brief formal definition in Section 2 would improve readability.
Circularity Check
No significant circularity: the ER-symmetry discovery fit and the reported zero-shot coordination results are evaluated on disjoint policy sets, so the headline cross-play numbers are not forced by the fitting procedure.
full rationale
The paper defines Phi_ER (Definition 4) as transformations preserving the set Pi_alpha* of self-play-optimal Boltzmann-exploratory policies. While this definition is tailored to self-play-optimal policies, the reported zero-shot coordination improvements are not obtained by re-evaluating the same policies used to fit the symmetries: agents first discover transformations on a fixed pool Pi' of SP-optimal policies (Eqs. 8-11, Algorithms 1-3), then train new OP_Phi_ER policies via Eq. 4, and finally cross-play among these independently retrained policies is measured (Sections 4.1-4.4). The OP_Phi_ER values in Section 4.4 (23.59 vs 23.34) are a post-hoc check on OP-optimal policies, not quantities that enter the symmetry-selection objective. The paper's own limitation statement (Section 6) notes dependence on the policy type used for discovery and on the bijective action/observation parameterization; these are scope and correctness constraints, not evidence that the conclusion is equivalent to its inputs. The main theoretical gap identified by a skeptical reader, namely that Definition 4 restricts Phi_ER to Pi_alpha* while OP is optimized over all policies, so the invariance guarantees need not transfer to OP_Phi_ER-optimal policies, is a validity concern about the strength of the theoretical link, not a circularity: the empirical cross-play results are not encoded in the definition or in the fitting objective. Self-citations, such as the use of a symmetrizer from Muglich et al. 2022a, are methodological prior work and are not load-bearing for the core claim. Thus no circular step can be exhibited from the paper's equations.
Assumptions & free parameters
free parameters (5)
- Boltzmann temperature alpha =
1 (three-lever, Hanabi), 1/2.667 (cat/dog), 1.1 (Overcooked V2)
- Regularization weights lambda_1, lambda_2 =
lambda_1 = 0.65, lambda_2 = 2.5e-9 (Hanabi)
- Pool sizes k, l, m =
k = 20/10/12/6, l = 6/3/16/11, m = 3/3/2/3 across environments
- Sampled action transpositions =
64 of 190 in Hanabi; exhaustive in smaller games
- phi_O,theta initialization and activation =
Identity-initialized linear layers with ReLU output
assumptions (6)
- standard math Standard Dec-POMDP model and Bellman equations define J, Q, and value functions.
- domain assumption Boltzmann-exploratory policies Pi_alpha are the right representative class of self-play optimal policies for defining expected return symmetries.
- domain assumption Actor-critic policies with entropy regularization converge to Boltzmann policies with logits proportional to Q-values.
- domain assumption The finite pool Pi-prime is representative of Pi_alpha*.
- ad hoc to paper Learned phi_O,theta can be treated as bijections on observation space.
- standard math The group Psi of bijective relabelings is finite, so every element has finite order.
Cite this review
Pith. "Pith review of Expected Return Symmetries." pith.science (2026). https://pith.science/paper/S6DUJ54Q
@misc{pith2026250201711,
author = {Pith},
title = {Pith review of: Expected Return Symmetries},
year = {2026},
howpublished = {\url{https://pith.science/paper/S6DUJ54Q}},
note = {Machine review of arXiv:2502.01711}
}
read the original abstract
Symmetry is an important inductive bias that can improve model robustness and generalization across many deep learning domains. In multi-agent settings, a priori known symmetries have been shown to address a fundamental coordination failure mode known as mutually incompatible symmetry breaking; e.g. in a game where two independent agents can choose to move "left'' or "right'', and where a reward of +1 or -1 is received when the agents choose the same action or different actions, respectively. However, the efficient and automatic discovery of environment symmetries, in particular for decentralized partially observable Markov decision processes, remains an open problem. Furthermore, environmental symmetry breaking constitutes only one type of coordination failure, which motivates the search for a more accessible and broader symmetry class. In this paper, we introduce such a broader group of previously unexplored symmetries, which we call expected return symmetries, which contains environment symmetries as a subgroup. We show that agents trained to be compatible under the group of expected return symmetries achieve better zero-shot coordination results than those using environment symmetries. As an additional benefit, our method makes minimal a priori assumptions about the structure of their environment and does not require access to ground truth symmetries.
Figures
Forward citations
Cited by 2 Pith papers
-
High entropy leads to symmetry-equivariant policies in Dec-POMDPs
Standard PPO with higher entropy and a tuned GAE reaches state-of-the-art cross-play between Hanabi seeds, but the stated proof that entropy forces symmetry-compatible policies is missing.
-
Is Inter-Seed Cross-Play Enough? Evaluating the Robustness of Zero-Shot Coordination Algorithms to Implementation Details
For Other-Play in Yokai, agents trained with different implementation details coordinate across implementations about as well as across seeds, supporting inter-seed cross-play as a proxy for cross-implementation evaluation.
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Reviewed August 9, 2026 · model on record in the stance chip above.
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