Generation and interrogation of a pure nuclear spin state by parahydrogen-enhanced NMR spectroscopy: a defined initial state for quantum computation

被引:27
作者
Blazina, D
Duckett, SB [1 ]
Halstead, TK
Kozak, CM
Taylor, RJK
Anwar, MS
Jones, JA
Carteret, HA
机构
[1] York Univ, Dept Chem, York YO10 5DD, N Yorkshire, England
[2] Univ Oxford, Clarendon Lab, Ctr Quantum Computat, Oxford OX1 3PU, England
[3] Univ Montreal, LITQ, Dept Informat & Rech Operationelle, Montreal, PQ H3C 3J7, Canada
关键词
NMR; HNMR; parahydrogen; photochemistry; quantum computing;
D O I
10.1002/mrc.1540
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We describe a number of studies used to establish that parahydrogen can be used to prepare a two-spin system in a pure state, which is suitable for implementing NMR quantum computation. States are generated by pulsed and continuous-wave (CW) UV laser initiation of a chemical reaction between Ru(CO)(3)(L-2) [where L-2 = dppe = 1,2-bis(diphenylphosphino)ethane or L-2 = dpae = 1,2-bis(diphenylarsino)ethane] with pure parahydrogen (generated at 18 K). This process forms Ru(CO)(2)(dppe)(H)(2) and Ru(CO)(2)(dpae)(H)(2) on a sub-microsecond time-scale. With the pulsed laser, the spin state of the hydride nuclei in Ru(CO)(2)(dppe)(H)(2) has a purity of 89.8 +/- 2.6% (from 12 measurements). To achieve comparable results by cooling would require a temperature of 6.6 mK, which is unmanageable in the liquid state, or an impractical magnetic field of 0.44 MT at room temperature. In the case of CW initiation, reduced state purities are observed due to natural signal relaxation even when a spin-lock is used to prevent dephasing. When Ru(CO)(3)(dpae) and pulsed laser excitation are utilized, the corresponding dihydride product spin state purity was determined as 106 +/- 4% of the theoretical maximum. In other words, the state prepared using Ru(CO)(3)(dpae) as the precursor is indistinguishable from a pure state. Copyright (C) 2004 John Wiley Sons, Ltd.
引用
收藏
页码:200 / 208
页数:9
相关论文
共 37 条
[1]   Preparing high purity initial states for nuclear magnetic resonance quantum computing [J].
Anwar, MS ;
Blazina, D ;
Carteret, HA ;
Duckett, SB ;
Halstead, TK ;
Jones, JA ;
Kozak, CM ;
Taylor, RJK .
PHYSICAL REVIEW LETTERS, 2004, 93 (04) :040501-1
[2]  
Bennett CH, 1996, PHYS REV A, V54, P3824, DOI 10.1103/PhysRevA.54.3824
[3]   Quantum information and computation [J].
Bennett, CH ;
DiVincenzo, DP .
NATURE, 2000, 404 (6775) :247-255
[4]   Purification of noisy entanglement and faithful teleportation via noisy channels [J].
Bennett, CH ;
Brassard, G ;
Popescu, S ;
Schumacher, B ;
Smolin, JA ;
Wootters, WK .
PHYSICAL REVIEW LETTERS, 1996, 76 (05) :722-725
[5]  
Bonhoeffer KF, 1929, Z PHYS CHEM B-CHEM E, V4, P113
[6]   TRANSFORMATION OF SYMMETRIZATION ORDER TO NUCLEAR-SPIN MAGNETIZATION BY CHEMICAL-REACTION AND NUCLEAR-MAGNETIC-RESONANCE [J].
BOWERS, CR ;
WEITEKAMP, DP .
PHYSICAL REVIEW LETTERS, 1986, 57 (21) :2645-2648
[7]   PARA-HYDROGEN AND SYNTHESIS ALLOW DRAMATICALLY ENHANCED NUCLEAR ALIGNMENT [J].
BOWERS, CR ;
WEITEKAMP, DP .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1987, 109 (18) :5541-5542
[8]  
BOWERS CR, 1990, ADV MAGN RESON, V14, P269, DOI DOI 10.1016/B978-0-12-025514-6.50018-6
[9]   Separability of very noisy mixed states and implications for NMR Quantum computing [J].
Braunstein, SL ;
Caves, CM ;
Jozsa, R ;
Linden, N ;
Popescu, S ;
Schack, R .
PHYSICAL REVIEW LETTERS, 1999, 83 (05) :1054-1057
[10]   Bulk quantum computation with nuclear magnetic resonance: theory and experiment [J].
Chuang, IL ;
Gershenfeld, N ;
Kubinec, MG ;
Leung, DW .
PROCEEDINGS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1998, 454 (1969) :447-467