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Muon-Adam: Hybrid Spectral-Adaptive Optimizer

Updated 5 July 2026
  • Muon-Adam is a hybrid optimization method that fuses spectral updates for matrices with Adam-style adaptive updates for vectors.
  • It combines exact matrix orthogonalization with adaptive moment estimation to induce an implicit bias toward max-margin solutions.
  • Practical performance relies on careful tuning of matrix and vector learning rates to balance spectral descent and adaptive coordinate updates.

Muon-Adam is a hybrid optimization scheme that combines Muon-style matrix orthogonalization with Adam-style adaptive coordinate updates. In the formulation analyzed for smooth homogeneous neural networks, parameters are partitioned as θ=(W1,,WK,u)\theta=(W_1,\dots,W_K,u), with Muon applied to matrix blocks WkW_k and Adam applied to the remaining vector block uu; the resulting dynamics are shown to induce an implicit bias toward Karush–Kuhn–Tucker (KKT) points of a hybrid max-margin problem (Gronich et al., 18 Feb 2026). A complementary non-Euclidean optimization perspective formulates the practical algorithm as constrained steepest descent in a mixed product norm, placing Muon-Adam within a broader family of spectral and adaptive methods (Crawshaw et al., 10 Oct 2025).

1. Definition and update structure

In the homogeneous-network analysis, Muon-Adam is studied on binary classification data {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\} with a smooth LL-homogeneous model f(x;θ)f(x;\theta), meaning f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta). The full-batch loss is

L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),

with (u)=eu\ell(u)=e^{-u} or (u)=log(1+eu)\ell(u)=\log(1+e^{-u}) (Gronich et al., 18 Feb 2026).

The parameter vector is partitioned as

WkW_k0

where each WkW_k1 is a matrix and WkW_k2 collects the remaining vector parameters. Muon-Adam then applies distinct update mechanisms to these two components. For the matrix blocks, it uses Muon with exact SVD orthogonalization; for the vector block, it uses Adam-style first- and second-moment adaptation. In continuous time, the matrix and vector dynamics are

WkW_k3

and

WkW_k4

where WkW_k5 is the subgradient block for WkW_k6, WkW_k7 is the subgradient for WkW_k8, and WkW_k9 denotes exact orthogonalization (Gronich et al., 18 Feb 2026).

A discrete practical formulation uses the same division of labor. Matrix layers uu0 are updated by

uu1

while non-matrix parameters uu2 use Adam buffers and the standard adaptive step

uu3

This formulation identifies Muon-Adam as a side-by-side composition of spectral descent for matrix blocks and Adam for the remaining parameters (Crawshaw et al., 10 Oct 2025).

2. Model assumptions and admissible trajectories

The implicit-bias theory for Muon-Adam is developed under a specific structural regime. The network must satisfy the smooth homogeneous assumptions uu4 and uu5 for some uu6. The loss uu7 must be strictly decreasing, twice-differentiable, and exponentially tailed, with logistic and exponential losses given as examples (Gronich et al., 18 Feb 2026).

The learning-rate schedule is also restricted. The base schedule uu8 must satisfy

uu9

and it must be non-increasing. These conditions ensure persistent motion while enforcing sufficient decay for the asymptotic steepest-descent approximation (Gronich et al., 18 Feb 2026).

Three trajectory assumptions are then imposed. First, the trajectory must be nontrivial, in the sense that eventually {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}0. Second, the direction must converge: {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}1 with positive margin {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}2. Third, Adam must be well-defined: on a short interval {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}3, all gradient squares exceed {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}4, ensuring {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}5 always (Gronich et al., 18 Feb 2026).

These are not generic optimizer assumptions; they define the scope in which the max-margin result is proved. A plausible implication is that Muon-Adam’s asymptotic characterization is most transparent in homogeneous models where directional convergence can be justified or observed empirically.

3. Hybrid norm geometry and steepest-descent interpretation

The central geometric object is a hybrid norm under which Muon-Adam behaves as an Approximate Steepest Descent (ASD) trajectory. In the homogeneous-model analysis, the relevant norm is

{(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}6

Its dual norm is

{(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}7

Thus the matrix part is governed by spectral/nuclear duality, while the vector part is governed by {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}8 duality (Gronich et al., 18 Feb 2026).

The ASD proof checks three conditions: the integrated step length diverges, the normalized step aligns asymptotically with the negative subgradient, and the size ratio satisfies {(xi,yi)}Rd×{±1}\{(x_i,y_i)\}\subset\mathbb R^d\times\{\pm1\}9. On the LL0-blocks, exact orthogonalization yields normalized momentum steepest descent for the spectral norm. On the LL1-block, the Adam ratio LL2 approximates the sign of LL3. The mixed dual norm selects the dominant nuclear-versus-LL4 contribution, and asymptotic alignment is recovered by partitioning time according to which component dominates (Gronich et al., 18 Feb 2026).

A related but distinct formulation casts practical Muon-Adam as constrained steepest descent in the infinity-product norm

LL5

In that view, the linear minimization oracle on each matrix block is LL6, and the LL7-block uses the Adam-style adaptive direction (Crawshaw et al., 10 Oct 2025). Taken together, these formulations place Muon-Adam at the intersection of spectral steepest descent and adaptive coordinate descent.

4. Max-margin bias and KKT characterization

The hard margin of a parameter vector is defined by

LL8

The associated max-margin problem under a norm LL9 is

f(x;θ)f(x;\theta)0

A point f(x;θ)f(x;\theta)1 with multipliers f(x;θ)f(x;\theta)2, subgradients f(x;θ)f(x;\theta)3, and f(x;θ)f(x;\theta)4 satisfies the KKT conditions if

f(x;θ)f(x;\theta)5

These conditions are the stationarity object to which Muon-Adam converges directionally (Gronich et al., 18 Feb 2026).

Once the ASD conditions are established and f(x;θ)f(x;\theta)6, the general KKT blueprint implies that any directional limit f(x;θ)f(x;\theta)7 is a KKT point of the hybrid-norm max-margin problem. The resulting margin is

f(x;θ)f(x;\theta)8

with the hybrid norm combining matrix spectral norms and the vector f(x;θ)f(x;\theta)9 norm (Gronich et al., 18 Feb 2026).

The main convergence statements make this explicit. Theorem 4.2 states that any ASD trajectory with asymptotic alignment and diverging norm converges directionally to a KKT point of the max-margin problem under the corresponding norm. Theorem 4.4 identifies Adam’s limit with a KKT point for f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)0. Theorem 4.6 states that Muon-Adam biases the hybrid max-spectral/f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)1 margin

f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)2

under the same homogeneity, decay, and directional-convergence assumptions (Gronich et al., 18 Feb 2026).

5. Relation to Adam, Muon-Signum, MomentumGD, and spectral families

Muon-Adam is one member of a family of momentum-based non-Euclidean optimizers whose implicit biases are determined by the norm geometry of their effective steepest-descent trajectories. Standard Adam, without the stability constant f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)3, is analyzed as maximizing the f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)4-margin. MomentumGD approximates normalized f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)5-steepest descent and biases the f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)6-margin. Muon-Signum, which applies Muon to matrices and Signum to vector parameters, biases the hybrid max-margin based on spectral norm for matrices and f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)7 for vectors. Muon-Adam “sits strictly between Muon-Signum (pure sign) and pure Adam,” because tuning f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)8 and f(x;αθ)=αLf(x;θ)f(x;\alpha\theta)=\alpha^L f(x;\theta)9 trades off spectral versus L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),0 influence in the hybrid norm (Gronich et al., 18 Feb 2026).

The non-Euclidean steepest-descent perspective sharpens this comparison. Muon-Adam is identified with constrained steepest descent, whereas MuonMax is derived from a regularized variant using an L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),1-style product norm. In that framework, Muon-Adam normalizes each matrix block individually by its polar factor and retains Adam on the remaining parameters, while MuonMax rescales matrix steps through a dual norm involving sums of nuclear norms (Crawshaw et al., 10 Oct 2025).

A broader unified spectral perspective places Muon and Adam at the endpoints of the spectral transform family

L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),2

with L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),3 corresponding to full orthogonalization and L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),4 corresponding to the identity transform. In the RMS-normalized case, L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),5 is exactly an Adam-style update, while L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),6 yields an AdamZ update. This suggests that Muon-Adam can be viewed as one concrete hybridization of two geometries that also admit interpolation at the level of singular-value compression (Qi et al., 4 Feb 2026).

6. Empirical behavior and practical profile

In the homogeneous-network experiments accompanying the implicit-bias analysis, Muon-Adam was evaluated on two-layer homogeneous nets trained on MNIST. The reported behavior follows the theoretical geometry: NGD and MomentumGD cause the L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),7-margin to rise fastest; Signum and Adam maximize the L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),8-margin; Muon maximizes the spectral-norm margin; and Muon-Adam yields the largest value of the hybrid margin

L(θ)=i=1m(yif(xi;θ)),L(\theta)=\sum_{i=1}^m \ell\bigl(y_i f(x_i;\theta)\bigr),9

The same experiments report cosine alignment of (u)=eu\ell(u)=e^{-u}0 to (u)=eu\ell(u)=e^{-u}1 above .99 in late training, supporting the directional-convergence assumption used in the theory (Gronich et al., 18 Feb 2026).

In language-model experiments from the non-Euclidean gradient study, Muon-Adam achieved mean validation loss (u)=eu\ell(u)=e^{-u}2 on FineWeb1B, while Muon-Adam + Momo achieved (u)=eu\ell(u)=e^{-u}3. The same study reports that plain Muon-Adam “requires precise tuning,” with factor-of-3 shifts in (u)=eu\ell(u)=e^{-u}4 or (u)=eu\ell(u)=e^{-u}5 capable of increasing validation loss by more than (u)=eu\ell(u)=e^{-u}6; adding Momo broadens the viable learning-rate region, and MuonMax-Momo is reported as the most robust variant on new tasks (Crawshaw et al., 10 Oct 2025).

These observations delimit Muon-Adam’s empirical profile. On the one hand, the hybrid optimizer realizes the norm-dependent margin behavior predicted by the ASD/KKT theory. On the other hand, its practical performance depends materially on the coupling between the matrix learning rate and the base Adam learning rate. This suggests that Muon-Adam is best understood not as a generic replacement for either parent optimizer, but as a geometrically structured hybrid whose behavior is controlled by the relative weight assigned to spectral and adaptive components.

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