KMS Fall Meeting, GIST
Neural-Network Wess-Zumino-Witten,
Duality and Machine Learning
Benjamin Suzzoni
2026/10/31
withPCPietro CapuozzoBRBrandon Robinson
A neural network is a composable map
Neural network:
\(\Phi_{\Theta}:\mathbb R^D\rightarrow\mathbb R\)
Operations: composition, addition and scalar multiplication.
Its functional form is the architecture; its weights and biases are the parameters.
one hidden layer
\[
\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad\Phi_{\Theta}(x)=\sum_i \Theta_i \varphi_i(x)
\]
The Universal Approximation Theorem (UAT)
one width parameter \(L\) controls both pictures
\(L=1\) width parameter; displayed nodes are schematic
coarse approximation schematic error
UAT: expressivity/density in a function space.
NNGP: a suitably normalized iid large-width limit can become Gaussian.
A functional integral through the UAT
Network at initialization: weights \(\Theta\) follow a distribution \(P\).
function space
\[
\int\mathcal D\phi\,\mu[\phi]\,\mathcal F[\phi]
\]
integrate over field configurations
↔
pushforward
through \(\Phi_\Theta\)
parameter space
\[
\lim_{L\to\infty}\int_{\Theta_L}
d\Theta\,P_L(\Theta)\,
\mathcal F[\Phi_\Theta]
\]
ordinary integrals over network parameters
Key Idea: replace the functional integral with a statistical average.
But: conformal correlators can already emerge at finite architecture—the UAT limit is not required to define an nn-CFT.
What has NNFT achieved?
T-duality identified in the bosonic-string setting
momentum↔winding
What about other dualities?
A 2d sigma model
\[g:\Sigma\longrightarrow SU(N)\]
worldsheet to group manifold
Affine current algebra
\[J^a(z)J^b(w)\sim\frac{K\delta^{ab}}{2(z-w)^2}+\frac{if^{ab}{}_{c}J^c(w)}{z-w}\]
Direct / coset
\[SU(N)_K\simeq\frac{SU(NK)_1}{SU(K)_N}\]
a common chiral current sector
The Wakimoto representation builds WZW currents from free fields.
neural free fields
\(\phi\) and \((\beta,\gamma)\)
one scalar, one commuting pair
Wakimoto readout
Polynomials and derivatives
with normal ordering
WZW observables
\(J^1,\ J^2,\ J^3\)
and the stress tensor \(T\)
One current, for example:\[J^3=i\sqrt{\frac{K+2}{2}}\,\partial\phi+:\!\beta\gamma\!:\]
The prescribed readouts reproduce the affine algebra in the ordered continuum limit.
One current sector, two neural presentations
The same limiting \(SU(2)_3\) sector, at the same feature width \(L\).
| Direct W \(SU(2)_3\) | Coset C \(SU(6)_1/SU(3)_2\) |
| Scalar fields | 1 | 5 |
| Commuting \(\beta\gamma\) pairs | 1 | 15 |
| Gaussian output amplitudes | \(3L\) | \(35L\) |
| Real sampled parameters | \(6L\) | \(38L\) |
| Observables retained | Three currents and the stress tensor |
Baseline shared frequencies and scalar phases. Count each complex frequency as two real parameters; fixed hyperparameters are excluded.
The continuum relation leaves different finite architectures and readouts.
Real life neural networks are not infinite...
what happens there?
Finite-width accuracy depends on the presentation
Compare stress-tensor correlations with the common CFT reference.
\(L\): feature width. \(\alpha\): spectral tilt at fixed elementary covariance.
UV damping (R¹)
Direct WCoset C
IR and UV damping (R³)
Direct WCoset C
\(\log_{10}E_X^{TT}\)white: resolved minimum
hatched: within 5%
Hover to inspect \(L\), \(\alpha\) and \(E^{TT}\). Same 64 pairs, \(p_-=.01\), \(p_+=1000\). Sampling uncertainty is separate.
Computational cost depends on the task
Coset / direct median CPU time, at \(L=256\), \(\alpha=0\), \(R^3\).
Ensemble-correlation workloadTime ratio (log scale)
1000 amplitude-dependent calls
1000 fixed-amplitude calls
Fixed coefficients allow more reuse. New insertion points require integration again.
A continuum identification does not select the most economical finite network.
These workloads evaluate ensemble correlations. Neither complete task reached the prescribed 1% full-vector accuracy target.
Thank you
Benjamin Suzzoni
with Pietro Capuozzo and Brandon Robinson