Crystal lattice quantum computer |
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Authors: | F Yamaguchi Y Yamamoto |
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Institution: | (1) Edward L. Ginzton Laboratory, Stanford University, Stanford, CA 94305-4085, USA (E-mail: fumiko@loki.stanford.edu), US;(2) NTT Basic Research Laboratories, 3-1 Morinosato-Wakamiya Atsugi, Kanagawa, 243-01, Japan, JP |
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Abstract: | 31 P nucleus can be used to represent a quantum bit (‘qubit’) with a relatively long relaxation time. In a CeP crystal lattice,
31P nuclei are periodically situated in three dimensions at distances of about 6 Å. The application of a static magnetic field
gradient in one direction causes differences in the Zeemanfrequencies of separate nuclei. This allows thousands of distinct
qubits to be individually addressed. Initializations of the qubits can be done efficiently by the Pound–Overhauser double
resonance effect on the nuclear spins and the antiferromagnetically ordered 4f electron spins of cerium ions. Logic operations
can be performed by simple pulse sequences, and computational results after logic operations can be measured by the nuclear
magnetic resonance of neighboring nuclei, or the electron resonance of neighboring 4f electrons of cerium ions.
Received: 26 October 1998/Accepted: 29 October 1998 |
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Keywords: | PACS: 03 67 Lx 76 60 k 75 50 Ee |
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