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Dec 9 at 4:18 comment added akkapi Note that the paper of Shukla & Vedula (arxiv.org/abs/2306.11747) achieves a superposition of computational basis states $| k_1 \rangle , \ldots, | k_M \rangle$ if $k_j = j - 1$, meaning only for the initial segment $[0, M - 1] \subset [0, 2^n - 1]$. The improvement over just Hadamard gates is that $M$ need not be a power of $2$ here. This doesn't quite answer the question of the OP, since there the subset can be arbitrary. Interestingly, this was recently overlooked elsewhere (see journals.aps.org/pra/pdf/10.1103/PhysRevA.110.056401) attempting to use Shukla-Vedula.
Apr 10 at 12:26 review Late answers
Apr 10 at 18:21
Apr 10 at 12:17 history edited Martin Vesely CC BY-SA 4.0
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S Apr 10 at 12:04 review First answers
Apr 10 at 18:20
S Apr 10 at 12:04 history answered Quantum_Brains CC BY-SA 4.0