2003
DOI: 10.1038/nature02015
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Demonstration of conditional gate operation using superconducting charge qubits

Abstract: Using a pulse technique, we prepare different input states and show that they can be transformed by controlled-NOT (C-NOT) gate operation in the amplitude of the states. Although the phase evolution during the gate operation is still to be clarified, the present results are a major step toward the realization of a universal solid-state quantum gate.

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Cited by 626 publications
(537 citation statements)
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“…There are two ways to control coefficients α and β: either change E J 1 by a magnetic field keeping t 1 constant [21], or change t 1 keeping E J 1 constant [62]. The latter case is technically more difficult as the length of the first pulse is changed while the second pulse is fixed.…”
Section: Quantum Logic Gatementioning
confidence: 99%
See 3 more Smart Citations
“…There are two ways to control coefficients α and β: either change E J 1 by a magnetic field keeping t 1 constant [21], or change t 1 keeping E J 1 constant [62]. The latter case is technically more difficult as the length of the first pulse is changed while the second pulse is fixed.…”
Section: Quantum Logic Gatementioning
confidence: 99%
“…[15], but with one more pulse gate, was also used for the demonstration of conditional gate operation [21]. Having two pulse gates enables us to address each qubit individually.…”
Section: Quantum Logic Gatementioning
confidence: 99%
See 2 more Smart Citations
“…We show that their physical properties simplify the implementation of the difficult steps mentioned above. In these systems one may use the charge 14,15,16 or the conjugate phase degree of freedom 17,18 to store and process quantum information. Typically, one adjusts the parameters such that the ground state is (almost) doubly degenerate, and at low energies the system reduces to a qubit.…”
Section: Introductionmentioning
confidence: 99%