For , the Pauli X gate and Pauli Z gate act on different qubits in , so they commute. Their product is a Hermitian matrix and squares to the identity operator. Its eigenvalues have modulus one; equivalently it is a unitary operator. Therefore its spectral norm isThe qualification is necessary because the qubit labelled one does not exist for .
The printed upper summation limit introduces although only qubits were defined. Literally the final term is undefined. Use the natural open-chain repairThis preserves the stated -qubit system and agrees with the supplied sum-of-squares hint. If a cyclic convention was intended instead, it must be stated; the same argument works for its terms when . For , the repaired open chain is empty and the target is the identity.
Here is a product-formula Hamiltonian simulation using exactly the two supplied lemmas. Let and choose an integer . Every is a norm-one Hermitian matrix. One time slice is the product of two-qubit gatesTo compare a partial product with , first propagate the previous error through the next unitary gate, which preserves the spectral norm, and then use Lemma A with , . Both norms are at most . Its new error is at most for a universal constant . For an explicit choice, follows from the unitary Taylor bounds and . Induction and the triangle inequality therefore giveLemma B, the unitary product telescoping bound, now compares the repeated slices with :Take, for example, . If the sum is zero the product is already exact; otherwise its error is at most . There are two-qubit gates. This explicit lemma-based construction has fourth-degree dependence on for fixed precision:This is a sufficient polynomial, not an optimality claim. The polynomial-degree statement treats as fixed; the inverse-precision dependence is displayed separately. No first-order term error is accumulated without the required repeated-slice factor.
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