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Pauli Decomposition by Character Theory: A Memory-Bounded Algorithm for Qubits and Qudits

Published 6 Oct 2026 in quant-ph | (2610.08299v1)

Abstract: Pauli decomposition underpins Trotterization, phase estimation, sparse-Hamiltonian simulation, and variational observables, at exponential naive cost. From the character theory of (Z2)<sup>n(\mathbb{Z}_2)<sup>n, characters χz(v)=(−1)<sup>⟨</sup>v,z⟩χ_z(v)=(-1)<sup>{\langle</sup> v,z\rangle} are the diagonal Pauli strings, so any diagonal operator is already Pauli-decomposed. A general operator still needs the shifts: each X<sup>⊗</sup>xX<sup>{\otimes</sup> x} couples to a character χz=Z<sup>⊗</sup>zχ_z=Z<sup>{\otimes</sup> z}, and the products X<sup>⊗</sup>xZ<sup>⊗</sup>zX<sup>{\otimes</sup> x}Z<sup>{\otimes</sup> z} -- up to phases in ±1,±i{\pm 1,\pm i} -- form the Pauli group, the central extension of (Z2)<sup>n×(Z2)<sup>n(\mathbb{Z}_2)<sup>n\times(\mathbb{Z}_2)<sup>n by that phase group fixed by the symplectic pairing. A section of that extension remains a choice: the bare products X<sup>⊗</sup>xZ<sup>⊗</sup>zX<sup>{\otimes</sup> x}Z<sup>{\otimes</sup> z}, or the genuine operators that insert Y=iXZY=iXZ at every qubit where xx and zz overlap. As Fourier analysis on an abelian shift-character lattice (a natural DFT), this formulation is not qubit-bound: (Zp)<sup>n(\mathbb{Z}_p)<sup>n recovers Heisenberg-Weyl qudits. The fast algorithm is the FFT for the group at hand; on (Z2)<sup>n(\mathbb{Z}_2)<sup>n that FFT is Walsh-Hadamard, at cost O(n⋅4<sup>n)O(n\cdot 4<sup>n). paulikit is a memory-bounded realization of that qubit transform: peak usage need not materialize the dense 2<sup>n×</sup>2<sup>n2<sup>n\times</sup> 2<sup>n operator, unlike prior codes whose O(1)O(1) extra sits on that buffer, checked beyond a billion oscillator terms against Work-Span and bandwidth ceilings.

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