Sample-based quantum diagonalization (SQD) and quantum-selected configuration interaction (QSCI) are the electronic-structure methods with most hardware traction, yet their canonical target – the ground-state energy – is where classical methods have caught up. We move the target to dynamics and the resource question. From one bitstring-sampling primitive – computational-basis measurements of a shallow real-time circuit, with no Hadamard or controlled unitaries – we reconstruct, from sampled subspaces, the single-particle spectral functions and and the neutral-sector dynamical structure factors and , each built classically in the Lehmann representation from its own subspace. The reconstruction matches exact diagonalization on Hubbard chains and, for , across nineteen molecules (FCI-verified to Ha), and runs on the IBM Heron processor. Second, we ask which resource controls the cost – the determinant support the sampler must populate. On number-conserving states the fermionic AntiFlatness collapses to one 1-RDM invariant, . An orbital-rotation (Gaussian) invariant while is basis dependent, is provably decoupled from the cost; the cost is instead lower-bounded and tracked by the entanglement – the minimal bond dimension (Spearman ). One-body magic is thus a faithful multireference diagnostic but an unreliable cost predictor; any genuine advantage lives in the non-Gaussianity of the higher-body cumulants. We prove moment exactness and a sampling bound polynomial in , independent of Hilbert-space dimension. Self-consistent configuration recovery improves the subspace under device noise, while a learned generative model does not beat that classical baseline.

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