MixFunnQUANTUM DYNAMICS
Experiment 02 / Two qubits · S₂
EXPERIMENT 02 · SYMMETRIC SUBSPACE

Quantum dynamics of two qubits.

Exact evolution, neural approximation and Fourier operator continuation.

MixFunn · FNO · exact solution
PHYSICAL MODEL AND EVALUATIONExplore this experiment ↓

Interacting qubits in the symmetric sector

Two qubits experience equal local fields and a symmetric interaction tensor. The local terms rotate each qubit state, while the interaction terms can generate correlations and entanglement. The initial state is |00⟩ and ℏ = 1.

H=∑αhα(σαA+σαB)+∑αJαασαAσαB+∑α<βJαβ(σαAσβB+σβAσαB).\begin{aligned}H={}&\sum_{\alpha}h_\alpha(\sigma_\alpha^A+\sigma_\alpha^B)\\&+\sum_{\alpha}J_{\alpha\alpha}\sigma_\alpha^A\sigma_\alpha^B\\&+\sum_{\alpha<\beta}J_{\alpha\beta}(\sigma_\alpha^A\sigma_\beta^B+\sigma_\beta^A\sigma_\alpha^B).\end{aligned}

Here σαA=σα⊗I\sigma_\alpha^A=\sigma_\alpha\otimes I and σαB=I⊗σα\sigma_\alpha^B=I\otimes\sigma_\alpha act on Qubit A and Qubit B, respectively; α,β∈{x,y,z}\alpha,\beta\in\{x,y,z\}.

Exchange symmetry preserves the triplet basis {|00⟩, (|01⟩ + |10⟩)/√2, |11⟩}. Three complex amplitudes therefore determine the state throughout the evolution. The fields are (0.50, 0.51, 0.49), the diagonal couplings are (0.20, 0.21, 0.19), and (Jxy, Jxz, Jyz) = (0.05, 0.06, 0.04).

Two qubits connected by an interaction, each subject to an equal local field.
Schematic representation. The orange arrows indicate local effective fields. Equal fields on both sites preserve exchange symmetry.

Neural representation and temporal continuation

A MixFunn network [1] approximates the triplet amplitudes over 0 ≤ t ≤ 10. The two variants compare training with supervised QuTiP observables and training with physical constraints alone. A Fourier neural operator then advances temporal windows using the approach of Shah et al. [2]. In this experiment, both its input and target windows come from MixFunn trajectories.

Parameters and observables

The controls select the training variant, visible methods, curve colors, observable and viewing interval. The Hamiltonian coefficients remain fixed for these trained networks. Computational basis probabilities resolve the four measurement outcomes. The XX, YY and ZZ correlators describe joint Pauli measurements along a common axis; a nonzero correlator alone does not establish entanglement.

The fidelity panel compares normalized predicted states with the exact trajectory. Continuation is available to t = 50 for the variant with data and t = 20 for the variant without supervised data. Shading begins at t = 10. The time cursor selects a state snapshot within the chosen interval.

INTERACTIVE EXPERIMENT

Parameters and quantum evolution

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