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REVIEW 4 major objections 5 minor 1 cited by

Pushing the Limits of Low-Bit Optimizers: A Focus on EMA Dynamics

T0 review · 4 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash

Pith's one-line read The paper demonstrates that Adam-style optimizers can keep their state in as few as 2-3 bits per value without meaningful accuracy loss, by fixing two EMA-specific quantization failures: signal swamping in unsigned states and inflated…

desk verdict SOLO's 4/2-bit optimizer is a solid, well-tested contribution; the 2-bit claim leans on a heuristic momentum rule that the paper itself doesn't fully support. read the letter →

arxiv 2505.00347 v2 pith:ZPNXSEK2 submitted 2025-05-01 cs.LG cs.AI

classification cs.LGcs.AI
keywords low-bitoptimizersAdamquantizationEMAdynamicssignalswampinggradientvariancestochasticroundingmemory-efficienttraining
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

SOLO claims that Adam-style optimizers can store their state in as few as 3 or even 2 bits per value instead of 32, with only marginal accuracy loss. The reason previous 4-bit attempts degraded is that they ignored the exponential moving average (EMA) dynamics: nearest-rounding quantization freezes the unsigned second-moment state ("signal swamping"), and signed first-moment quantization inflates gradient variance enough to reverse descent. The fix is a logarithmic quantizer with stochastic rounding for the unsigned state, plus a smaller momentum hyperparameter for the signed state, chosen from a variance bound. On benchmarks spanning computer vision, translation, recommendation, and LLM/LVM fine-tuning, the 4/2-bit variant is statistically indistinguishable from full-precision Adam (Wilcoxon p=0.125 on MMLU-style tasks), and a fully 2-bit version remains competitive. If correct, this cuts optimizer memory by roughly an order of magnitude, making large-model training feasible on much smaller GPU budgets.

What carries the argument

The load-bearing object is the quantized EMA update: $\tilde{x}_t = Q^\dagger(q_t)$, then $\hat{x}_{t+1} = \beta\tilde{x}_t + (1-\beta)z_{t+1}$, then $q_{t+1}=Q(\hat{x}_{t+1})$, where $z_{t+1}$ is the gradient (signed) or squared gradient (unsigned). Two results extracted from this loop do the work. Theorem 3.1 states that the quantized level stays fixed whenever the level radius satisfies $r \ge (1-\beta)|\frac{z_{t+1}}{\Delta_{t+1}} - y_{q_t}| + |\frac{\Delta_t}{\Delta_{t+1}}-1|$, which identifies why standard quantizers fail at low precision and large tensor size. Theorem 3.6 proves that signed-state quantization inflates gradient variance by at most $\big(\frac{\beta}{1-\beta} r_{\max}(b)\Delta_t\big)^2$, which motivates the $\beta'$ adjustment rule of Eq. (15) using $r_{\mathrm{median}}$. The closing piece is the logarithmic quantizer of Eq. (10), $Q(x)=\mathrm{Clip}(\lfloor \log_\alpha(x/\Delta)+\xi\rceil;0,2^b-1)$ with $\alpha=(x_p/\Delta)^{1/(2^b-1)}$ and $\xi\sim U[-0.5,0.5]$, which prevents swamping and matches EMA decay.

What would settle it

Run the recommended 2-bit settings ($\beta'=0.527$ for fine-tuning, lower for scratch) on a large-scale pretraining run the paper leaves untested, e.g., a 175B model; if loss diverges or the accuracy gap exceeds the fine-tuning margins, the variance-regulation hypothesis fails. A cheaper check: directly measure gradient variance under 2-bit signed quantization and compare it with the bound in Eq. (14) and the claimed $r_{\mathrm{median}}/r_{\max}$ ratio similarity.

Watch

Extended reading notes

Core claim

The paper's central claim is that ultra-low-bit quantization of Adam is possible when the EMA state update is treated as a dequantize-EMA-quantize loop, and two mechanisms are added. For the unsigned second moment, Theorem 3.1 gives a precise signal-swamping condition: if the quantization radius around the current level is large enough, the state stays constant even when the incoming signal differs sharply; the paper shows this occurs at momentum values as low as $\beta \approx 0.833$ for 2-bit linear quantization. Its remedy is a logarithmic quantizer with levels clustered near zero, base $\alpha = (x_p/\Delta)^{1/(2^b-1)}$, and stochastic rounding, which also reproduces the exact expected decay time under consecutive zero signals. For the signed first moment, Theorem 3.6 bounds the added gradient variance by $\big(\frac{\beta}{1-\beta} r_{\max}(b)\Delta_t\big)^2$, and SOLO chooses a lower momentum $\beta'$ so that $\frac{\beta'}{1-\beta'} r_{\mathrm{median}}(b') \le \frac{\beta}{1-\beta} r_{\mathrm{median}}(b)$, giving $\beta' \le 0.820$ for 4-bit fine-tuning and $\beta' \le 0.527$ for 2-bit. The resulting 4/2-bit AdamW matches 32-bit AdamW within statistical noise on the evaluated tasks.

Load-bearing premise

The central claim depends on the hypothesis that bringing the quantization-induced gradient-variance upper bound under control is enough to keep convergence acceptable: the paper states this as a hypothesis rather than a theorem, and the recommended $\beta'$ values are chosen from empirical observation on the evaluated tasks, not from a convergence proof.

Editorial extensions

If this is right

  • Optimizer memory for Adam drops to about one-eighth (4/2-bit) or one-sixteenth (2-bit) of the 32-bit state size, letting practitioners fit larger models or batches on the same hardware.
  • Existing learning rates and weight decay remain unchanged; only the first-moment momentum needs lowering, to 0.8 for 4/2-bit and 0.5 for 2-bit fine-tuning, and to 0.3/0.1 for training from scratch.
  • The quantization scheme is model- and task-agnostic in the tested regimes: it transfers across Swin-T, Transformer-Base, RoBERTa-L, DCN, HSTU, LLaMA-7B/13B/33B, and LLaVA-1.5, and also covers the AdaBelief optimizer.
  • The logarithmic quantizer preserves second-moment dynamics when the block size is increased from 128 to 2048, unlike linear or dynamic-exponent quantizers that collapse, so per-block scale-factor overhead can be nearly eliminated.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • This suggests the momentum-reduction recipe could carry over to other EMA-based optimizers such as Lion or Adafactor, since the variance bound comes from the EMA loop rather than from Adam's specifics.
  • The signal-swamping condition implies a general design rule for low-bit states that feed a denominator: allocate quantization levels near zero and use stochastic rounding; this could inform low-bit batch-normalization statistics or embedding-table scalers.
  • The p-quantile base selection appears transferable to fully quantized training of weights and activations, where small-magnitude values dominate, but this would require independent validation.
  • The reported equivalence holds on only five MMLU-style benchmarks; extending the comparison to a larger suite with repeated seeds would test whether the "no significant difference" claim generalizes.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

4 major / 5 minor

Summary. The paper introduces SOLO, a low-bit optimizer-state quantization method that aims to maintain Adam-style optimizer states at 3-bit or even 2-bit precision with minimal accuracy loss. The authors identify two problems with naive low-bit quantization: signal swamping in unsigned EMA updates of the second moment, and increased gradient variance in signed EMA updates of the first moment. They address swamping with a logarithmic quantization scheme whose base is set by a p-quantile and which admits a simple stochastic-rounding implementation with an exact exponential-decay property. They address the gradient-variance issue by proposing a reduced first-moment momentum β' selected through an inequality (Eq. 15) that compares quantization radii at different precisions. The method is evaluated across CV, NLP, recommender systems, LLM instruction tuning, and LVM visual instruction tuning, with the 4/2-bit variant and a fully 2-bit variant compared against 32-bit, 16-bit, 8-bit, and 4-bit AdamW baselines. The paper also reports a robustness study of block-size choice and p-quantile sensitivity.

Significance. If the results hold, SOLO is a significant advance: it would reduce optimizer memory by roughly 10x relative to 32-bit AdamW while keeping performance close to full precision, and it is orthogonal to model architecture and distributed training. The unsigned logarithmic quantization with the p-quantile base is a clean and useful contribution, particularly because it preserves state dynamics under sparse-gradient and zero-signal conditions. The paper is transparent about its limitations, explicitly labels the momentum-reduction rule as a hypothesis, releases code, and reports broad experiments including LLaMA-13B/33B and LLaVA-1.5. The main weakness is that the load-bearing recipe for β'—the signed-momentum adjustment that makes 2-bit states workable—is a heuristic whose stated justification contains a numerically false 'nearly identical' ratio claim and whose variance analysis omits the EMA estimator's own variance increase when β is reduced. These issues are fixable but require substantive revision.

major comments (4)
  1. [Section 3.3, Eq. (15), Fact A.1, Figure 4] The assertion that the ratio r*(b)/r*(b') is 'nearly identical' for the median and maximum radius is contradicted by the paper's own Fact A.1 for signed DE quantization. For example, using the reported values, r_med(5)/r_med(2)=0.034/0.275≈0.124, while r_max(5)/r_max(2)=0.056/0.275≈0.204, a difference of roughly 1.65x. Since Theorem 3.6 bounds the quantization-induced variance in terms of r_max, replacing r_max by r_median in Eq. (15) is not a cosmetic change; the 'upper bounds' shown in Figure 4 are not consequences of the theorem. The authors should either re-derive the inequality with r_max and adjust the recommended β' values, or explicitly present Eq. (15) as an empirical heuristic and remove the 'nearly identical' claim.
  2. [Section 3.3, Eq. (14), Figure 6] The variance analysis in Eq. (14) accounts only for the quantization-induced noise term and omits the effect of reducing β on the EMA estimator's own variance. For a stationary gradient with variance σ², the first-moment estimate has variance proportional to (1-β)/(1+β); reducing β from 0.9 to 0.5 increases this component by roughly a factor of 6, which can offset the reduction in the quantization-noise term. The empirical optimum at β'≈0.5 in Figure 6 therefore does not follow from Eq. (14). The authors should provide a complete variance tradeoff for the momentum choice, including the estimator-variance term, or explicitly rephrase the Section 3.3 rationale as empirically motivated rather than derived.
  3. [Section 3.3, Theorem 3.6] Theorem 3.6's unbiasedness result, Eq. (13), relies on stochastic rounding, as the proof notes, but the manuscript does not state whether the signed DE quantization used in the experiments employs stochastic rounding. If nearest rounding is used, E[\tilde{g}] ≠ E[g] and the variance bound in Eq. (14) is not directly applicable. Please state the rounding scheme used for signed states; if it is not stochastic rounding, extend the analysis to cover the resulting bias or provide empirical evidence that the bias is negligible for the reported settings.
  4. [Tables 1-2, Section 4.1] Several 2-bit results show visible drops relative to 32-bit AdamW that are not discussed: HSTU HR 32.73→32.03, LLaVA ScienceQA 70.81→69.51, and LLaMA SIQA 48.50→47.21. The Wilcoxon signed-rank tests are based on only five metrics and are underpowered, so 'no statistically significant difference' (p=0.125 and p=0.285) should not be presented as evidence of equivalence. Please discuss these exceptions explicitly and soften the 'minimal accuracy loss' phrasing for the 2-bit setting, or provide additional runs and confidence intervals to support the claim.
minor comments (5)
  1. [Table 2 captions] The phrase 'ap-vlue' should read 'p-value'.
  2. [Eq. (10)] The notation ⌊·⌉ for convergent rounding is used without definition in the main text; please define it where Eq. (10) is introduced.
  3. [Figure 3 caption] The caption and subfigure text are dense and difficult to parse; consider splitting the figure into two panels with clearer labels for the quantization levels and the p-quantile mechanism.
  4. [Appendix C.1, Table 9] The word 'utlize' should be 'utilize'.
  5. [Section 3.3, Figure 4] If Eq. (15) is a heuristic rather than a proven upper bound, the figure caption should state this explicitly to avoid overstating the theoretical grounding.

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity: SOLO's design and recommended beta' are either derived from explicit quantization-geometry arguments or openly labeled as empirical hypotheses, not as predictions forced by fitted inputs.

full rationale

The paper's two central design choices are not circular. The unsigned logarithmic quantizer follows from the signal-swamping bound (Theorem 3.1, Corollary 3.2) and the variance analysis of stochastic rounding near zero (Proposition 3.4); the choice of base alpha=(x_p/Delta)^(1/(2^b-1)) is a separate quantile-adaptive construction that is tested for sensitivity (Figure 8, Table 11), not derived from the final accuracy numbers. The signed-momentum adjustment is openly presented as a hypothesis: Section 3.3 states 'we hypothesize that an acceptable convergence rate could be achieved once the upper bound is somewhat regulated' and Eq. (15) is a regulation criterion, not a theorem; the paper then tests beta' values empirically (Figure 6, Table 12). No self-citations are load-bearing—the citations to Higham, Oh, Xia, Dettmers, Li, etc. are external and do not supply the paper's own claims. The hyperparameters p=0.1 and the default beta' values are disclosed as empirical settings ('based on Figure 4 and empirical observations', 'for simplicity'), so they are not secretly fitted quantities relabeled as predictions. The paper also honestly flags an important limitation: large-scale pretraining 'remains unverified due to prohibitive computational costs', which is a scope restriction rather than a circular move. The r_median-vs-r_max ratio statement in Section 3.3 is not fully supported by Fact A.1 (2-bit signed DE gives r_med ratio approximately 0.0145 versus r_max ratio approximately 0.0255), but this is an internal-consistency/correctness concern, not a circularity: Eq. (15) would still be a non-tautological heuristic. Overall, the derivation chain is self-contained and empirically anchored; there are no steps in which an output quantity equals an input by construction.

Assumptions & free parameters 2 free parameters · 4 assumptions · 0 invented entities

The central method introduces two tuned hyperparameters, p and β', and relies on two domain assumptions plus two paper-specific heuristics: variance-regulation sufficiency and the r_median substitution. No new physical or mathematical entities are postulated.

free parameters (2)
  • p-quantile p = 0.1 (fixed); effective range reported as [0.05, 0.3]
    The logarithmic quantization base α = (x_p/Δ)^(1/(2^b-1)) uses the p-quantile x_p of the tensor. The paper states 'Empirically, a value of p∈[0.05,0.3] has been found to be effective across various scenarios' and fixes p=0.1. This determines the quantization levels and affects the second-moment dynamics, so the central claim depends on it.
  • first-moment momentum β' = 4/2-bit: 0.8 (fine-tune), 0.3 (scratch); 2-bit: 0.5 (fine-tune), 0.1 (scratch)
    β' is recommended via Eq. (15), but using r_median and 'empirical observations'. The specific values are chosen to stabilize training on the evaluated tasks, making them effectively tuned hyperparameters rather than purely derived predictions.
assumptions (4)
  • standard math Stochastic rounding has zero-mean quantization error
    Invoked in the proof of Theorem 3.6 to claim E[g̃_{t+1}] = E[g_{t+1}] (Eq. 13). This is a standard property of stochastic rounding (Xia et al., 2020).
  • domain assumption Reducing gradient variance improves convergence
    The paper justifies the momentum reduction by citing Li et al. (2023b) and Wang et al. (2024) to argue that lower gradient variance helps convergence. This is an external result about stochastic optimization, assumed without re-derivation.
  • ad hoc to paper Variance-upper-bound regulation is sufficient for acceptable convergence
    Section 3.3: 'we hypothesize that an acceptable convergence rate could be achieved once the upper bound is somewhat regulated', leading to Eq. (15). This is the load-bearing heuristic behind all β' recommendations and is not proven.
  • ad hoc to paper r_median approximates r_max for the ratio in Eq. (15)
    Section 3.3 states that the ratio of r*(b)/r*(b') is 'nearly identical' for median and maximum radius, justifying the substitution. No proof is given, and it affects all recommended β' values.

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Cite this review

Pith. "Pith review of Pushing the Limits of Low-Bit Optimizers: A Focus on EMA Dynamics." pith.science (2026). https://pith.science/paper/ZPNXSEK2

@misc{pith2026250500347,
  author       = {Pith},
  title        = {Pith review of: Pushing the Limits of Low-Bit Optimizers: A Focus on EMA Dynamics},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/ZPNXSEK2}},
  note         = {Machine review of arXiv:2505.00347}
}
read the original abstract

The rapid scaling of models has led to prohibitively high training and fine-tuning costs. A major factor accounting for memory consumption is the widespread use of stateful optimizers (e.g., Adam), which maintain auxiliary information of even 2x the model size in order to achieve optimal convergence. We therefore present SOLO in this work to spawn a novel type of optimizer that requires an extremely light memory footprint. While previous efforts have achieved certain success in 8-bit or 4-bit cases, SOLO enables Adam-style optimizers to maintain quantized states with precision as low as 3 bits, or even 2 bits. This immense progress is due to the identification and resolution of two key challenges: the signal swamping problem in unsigned quantization that results in unchanged state dynamics, and the increased gradient variance in signed quantization that leads to incorrect descent directions. The theoretical analysis suggests a tailored logarithmic quantization for the former and a precision-specific momentum hyperparameter for the latter. SOLO can thus be seamlessly applied to Adam-style optimizers, leading to substantial memory savings with minimal accuracy loss.

Figures

Figures reproduced from arXiv: 2505.00347 by the authors.

Figure 1
Figure 1. Memory costs of frontier LLMs, from left to right in￾cluding Touvron et al. (2023); Yang et al. (2024); Radford (2018); GenAI (2023); Anil et al. (2023); Liu et al. (2024b). The costs are estimated based on a standard mixed-precision training: 1) 16-bit model weights along with a 32-bit copy; 2) 16-bit gradients; 3) 32-bit optimizer states. Other activations and temporary buffers are excluded for simplicity. 2024a))… view at source ↗
Figure 2
Figure 2. Synthetic uniform signals. E[z] = 0.5 represents the expected value to which the quantized state shall converge. grow to an unacceptable level. To provide a clearer under￾standing of this impact, we demonstrate several surprising cases associated with two widely adopted quantization meth￾ods. As the unsigned EMA state update is most affected, we present the analysis on unsigned quantization and leave a generalized v… view at source ↗
Figure 3
Figure 3. (a) Comparison of various quantization approaches: The proposed allocates a greater number of quantization levels near the zero point, effectively reducing variance. (b) Illustration of 2-bit unsigned quantization: 2-digit precision number is shown for clarity. used linear or dynamic exponent quantization methods may not be well-suited in this scenario, as they fail to adequately account for this consideration. As s… view at source ↗
Figures from the paper (10 more)
Figure 4
Figure 4. Figure 4: The upper bound of β ′ for DE according to Eq. (15). As a result, training failures are frequently observed in low￾precision quantization, particularly in cases where training begins from scratch. To summarize, The signed EMA update, in particular for training from scr…
Figure 5
Figure 5. Figure 5: Block size generalizability. The top panel reports the results fine-tuned with a 4/2-bit AdamW whose 2nd EMA update is quantized by DE, Linear (excluding the zero point), and the tailored logarithmic quantization. The bottom panel illustrates how the 2nd state distribu…
Figure 6
Figure 6. Figure 6 [PITH_FULL_IMAGE:figures/full_fig_p010_6.png]
Figure 7
Figure 7. Figure 7: The training loss on LLaMA fine-tuning. • AdaBelief. Although the results in [PITH_FULL_IMAGE:figures/full_fig_p011_7.png]
Figure 8
Figure 8. Figure 8: Sensitivity analysis of p-quantile. For clarity, we illus￾trate the differences relative to the default value of p = 0.1. model fine-tuned with 4/2-bit AdamW performs optimally at β1 = 0.8 or 0.9, and its performance deteriorates as β1 decreases. Conversely, the perfor…
Figure 9
Figure 9. Figure 9: Linear and DE mappings for unsigned and signed cases. A. Quantization Methods In this part, we provide a detailed introduction to the aforementioned Linear and Dynamic Exponent (DE) quantization techniques. Particular emphasis is placed on the following mapping formula…
Figure 10
Figure 10. Figure 10: How the 2nd state distribution of Transformer-Base ( ) changes at steps 50, 100, 150, and 200. DE quantization is omitted, as it leads to an immediate training collapse. 24 [PITH_FULL_IMAGE:figures/full_fig_p024_10.png]
Figure 11
Figure 11. Figure 11: How the 2nd state distribution of RoBERTa-Large ( on COLA) changes at steps 50, 100, 150, and 200. 25 [PITH_FULL_IMAGE:figures/full_fig_p025_11.png]
Figure 12
Figure 12. Figure 12: How the 2nd state distribution of DCN ( ) changes at steps 50, 100, 150, and 200. 26 [PITH_FULL_IMAGE:figures/full_fig_p026_12.png]
Figure 13
Figure 13. Figure 13: How the 2nd state distribution of HSTU ( ) changes at steps 50, 100, 150, and 200. 27 [PITH_FULL_IMAGE:figures/full_fig_p027_13.png]

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Pith tools

Reviewed August 16, 2026 · model on record in the stance chip above.