Result 1: necessary and sufficient fast-control simulation
OpenQAlgorithms.Papers.Independent.Intakethird100.P99.simulation_iff_integerShiftLet be a Hermitian Hamiltonian on two qubits , with canonical interaction coefficients satisfying . Local terms in are allowed. Local unitary controls are instantaneous and free, interaction intervals are nonnegative, and . Write for the infimum of the interaction durations of protocols implementing the gate , allowing the ideal limit of arbitrarily fine pulses at fixed total duration and disregarding global phase. This cost is an extended nonnegative real, with value for an impossible simulation. For a two-qubit unitary , let be an actual interaction-content witness: is locally equivalent, up to global phase, to , where are the Pauli matrices and . For real triples, means s-majorization: sort their absolute coordinates in descending order, give the smallest coordinate the sign of the product, and compare the first coordinate and the two sums . For every ,
The protocol is an operator protocol uniform over all input states. This is a two-way feasibility characterization, including .
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P99
namespace QAlgorithms.Papers.Independent.Intakethird100.P99
open scoped Matrix Kronecker NNReal ENNReal
open QAlgorithms.Papers.Independent.Information100.P10 (pauli)
open QAlgorithms.Papers.Independent.Information100.P32 (evolution)
noncomputable section
/-- PDF pp.4–6, Result 1: exact ideal fast-control feasibility iff some integer shift is
s-majorized by the available canonical interaction-time vector, also at time zero. -/
theorem simulation_iff_integerShift (H U : TwoMatrix) (a b : Triple) (t : ℝ)
(hH : HasCanonicalHamiltonian H a) (hU : HasContent U b) (ht : 0 ≤ t) :
IdealSimulates H U t ↔ ∃ n : Fin 3 → ℤ, SMajorized (contentIntegerShift b n) (t • a) := by sorry
end
end QAlgorithms.Papers.Independent.Intakethird100.P99
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What the Lean code literally says, in plain math · gpt-6.1-sol
For every pair of complex two-qubit matrices , real triples , and real , assume that is Hermitian, , , and there exist single-qubit unitary matrices and Hermitian single-qubit matrices such that , where and are the standard Pauli matrices. Assume also that is unitary, , , , and for some single-qubit unitaries . For any real triple , let have first coordinate , second coordinate , and third coordinate if , or otherwise; define by
Then the following are equivalent: for every real , there exist a finite list of nonnegative durations , single-qubit unitary matrices for , and with , such that and
and there exists an integer triple such that
The finite list may be empty, the time is included, and there is no positivity assumption on beyond the stated ordering conditions.
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.