2005
DOI: 10.1016/j.jmr.2005.04.009
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Quantum logical operations for spin 3/2 quadrupolar nuclei monitored by quantum state tomography

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Cited by 26 publications
(45 citation statements)
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“…(18a)-(18j), where we do not have distinct spectral densities for each qubit. We recall that we can consider this I = 3/2 system as an effective two-qubit one since we can manipulate the transitions between the energy levels of these logical qubits (i.e., the nuclear transitions of the quadrupolar spin) just as it is performed in the case of physical qubits [43].…”
Section: Fig 2 (Color Online)mentioning
confidence: 99%
“…(18a)-(18j), where we do not have distinct spectral densities for each qubit. We recall that we can consider this I = 3/2 system as an effective two-qubit one since we can manipulate the transitions between the energy levels of these logical qubits (i.e., the nuclear transitions of the quadrupolar spin) just as it is performed in the case of physical qubits [43].…”
Section: Fig 2 (Color Online)mentioning
confidence: 99%
“…Together with proper temporal or spatial averaging procedures and evolution under spin interactions [23], the RF pulse can be specially designed to prepare any two-qubit computational base states, as well as their superpositions, starting from the thermal equilibrium state [2,[24][25][26].…”
Section: Measuring Quantum and Classical Correlations In Nuclear Magnmentioning
confidence: 99%
“…From the application of a sequence of such pulses, by setting the pulses duration, phase and amplitude, a very fine control over the density matrix population and coherences can be achieved, and it is possible to generate all two-qubit computational base states, also superposition and entangled states [22,29]. It is important to note that these entangled states are called pseudo-entangled states because ǫ ∼ 10 −5 , which makes ρ pps always separable even when ρ 1 is an entagled state [32].…”
Section: Nmr Two Qubit Systemsmentioning
confidence: 99%