State Transfer and Spin Measurement

dc.creatorKay, A.
dc.date2006-04-19
dc.date2006-04-21
dc.date.accessioned2026-07-07T07:41:08Z
dc.date.available2026-07-07T07:41:08Z
dc.descriptionWe present a Hamiltonian that can be used for amplifying the signal from a quantum state, enabling the measurement of a macroscopic observable to determine the state of a single spin. We prove a general mapping between this Hamiltonian and an exchange Hamiltonian for arbitrary coupling strengths and local magnetic fields. This facilitates the use of existing schemes for perfect state transfer to give perfect amplification. We further prove a link between the evolution of this fixed Hamiltonian and classical Cellular Automata, thereby unifying previous approaches to this amplification task. Finally, we show how to use the new Hamiltonian for perfect state transfer in the, to date, unique scenario where total spin is not conserved during the evolution, and demonstrate that this yields a significantly different response in the presence of decoherence.
dc.description4 pages, 2 figures
dc.identifierhttps://arxiv.org/abs/quant-ph/0604137
dc.identifierhttp://arxiv.org/abs/quant-ph/0604137
dc.identifierPhys. Rev. Lett. 98, 010501 (2007)
dc.identifierdoi:10.1103/PhysRevLett.98.010501
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/121992
dc.subjectQuantum Physics
dc.titleState Transfer and Spin Measurement
dc.typetext

Files

Collections