Were the NMR machines of the 1980's performing a rudimentary quantum computation with phase cycling?
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In his 1996 paper Universal Quantum Simulators Seth Lloyd continues to formalize the problem of Hamiltonian simulation, showing that local Hamiltonian simulation is in BQP by applying the Baker-Campbell-Hausdorff formula to a Trotterization of the evolution. I particularly like his analogy between rapidly switching among noncommuting Pauli operators and rapidly going forward and backward to parallel park a car. In the paper Lloyd comments that this technique is familiar in NMR spectroscopy, poin
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Were the NMR machines of the 1980's performing a rudimentary quantum computation with phase cycling?
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In his 1996 paper Universal Quantum Simulators Seth Lloyd continues to formalize the problem of Hamiltonian simulation, showing that local Hamiltonian simulation is in BQP by applying the Baker-Campbell-Hausdorff formula to a Trotterization of the evolution. I particularly like his analogy between rapidly switching among noncommuting Pauli operators and rapidly going forward and backward to parallel park a car.
In the paper Lloyd comments that this technique is familiar in NMR spectroscopy, pointing to an early 1980 paper titled Theory of selective excitation of multiple‐quantum transitions by Warren, Weitekamp, and Pines (pdf here). They refer to their version of Trotterization as "phase cycling" - Figure 4 of that paper, reproduced below, is striking.
In view of the above, how much of a stretch is it to say that back in 1980, before Feynman's famous lecture, even the NMR scientists were discussing how to perform a 'quantum computation' using phase-cycling/Trotterization?
Or is the relation between these NMR scientists' discussion of phase cycling and Lloyd's discussion of Hamiltonian simulation more akin to that well-discussed relation between the Jacquard loom and the Babbage machine?
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Mark Spinelli
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