The relationship between ensemble quantum computing logical gates and NMR pulse sequence engineering exemplified by the SWAP operation

[1]  J. Bunkenborg,et al.  Doubling the sensitivity of natural abundance 13C– 13C INADEQUATE with off‐resonance compensation , 2000 .

[2]  J. Duus,et al.  Spin-State-Selective Excitation. Application for E.COSY-Type Measurement ofJHHCoupling Constants , 1997 .

[3]  Noah Linden,et al.  How to exchange information between two coupled nuclear spins: the universal SWAP operation , 1999 .

[4]  Arthur O. Pittenger,et al.  An Introduction to Quantum Computing Algorithms , 2000 .

[5]  Richard R. Ernst,et al.  Coherence transfer by isotropic mixing: Application to proton correlation spectroscopy , 1983 .

[6]  J. A. Jones,et al.  Quantum logic gates and nuclear magnetic resonance pulse sequences. , 1998, Journal of magnetic resonance.

[7]  Paul A. Keifer,et al.  Pure absorption gradient enhanced heteronuclear single quantum correlation spectroscopy with improved sensitivity , 1992 .

[8]  N. Gershenfeld,et al.  Bulk Spin-Resonance Quantum Computation , 1997, Science.

[9]  S. Glaser,et al.  Design of NMR pulse experiments with optimum sensitivity: coherence-order-selective transfer in I2S and I3S spin systems , 1998 .

[10]  N. Nielsen,et al.  A systematic strategy for design of optimum coherent experiments applied to efficient interconversion of double‐ and single‐quantum coherences in nuclear magnetic resonance , 1996 .

[11]  Arthur G. Palmer,et al.  Sensitivity improvement in proton-detected two-dimensional heteronuclear relay spectroscopy , 1991 .

[12]  T. Schulte-Herbrüggen,et al.  Clean TROSY: compensation for relaxation-induced artifacts. , 2000, Journal of magnetic resonance.

[13]  S. Glaser,et al.  Unitary control in quantum ensembles: maximizing signal intensity in coherent spectroscopy , 1998, Science.

[14]  O. W. Sørensen,et al.  I-spin n-quantum coherences in InS spin systems employed for E.COSY-type measurement of heteronuclear long-range coupling constants in NMR , 1997 .

[15]  David P. DiVincenzo,et al.  Quantum information and computation , 2000, Nature.

[16]  O. W. Sørensen,et al.  Polarization transfer experiments in high-resolution NMR spectroscopy , 1989 .

[17]  J. Briand,et al.  Double spin-state-selective coherence transfer. Application for twodimensional selection of multiplet components with long transverse relaxation times , 1998 .

[18]  D. Leibfritz,et al.  Accurate measurement of homonuclear coupling constants using JHH-TOCSY , 1992 .

[19]  O. W. Sørensen,et al.  Spin-state-selective coherence transfer via intermediate states of two-spin coherence in IS spin systems: Application to E.COSY-type measurement of J coupling constants , 1997 .

[20]  A. J. Shaka,et al.  Iterative schemes for bilinear operators; application to spin decoupling , 1988 .

[21]  R. R. Ernst,et al.  Reduction of multiplet complexity in COSY-type NMR spectra: The bilinear and planar COSY experiments , 1991 .

[22]  J. Briand,et al.  Simultaneous and Independent Rotations with Arbitrary Flip Angles and Phases for I, ISα, and ISβSpin Systems , 1998 .

[23]  Novel Pulse Sequences with Sensitivity Enhancement for In-phase Coherence Transfer Employing Pulsed Field Gradients , 1995 .

[24]  P. Wright,et al.  Sensitivity improvement in proton-detected two-dimensional heteronuclear correlation NMR spectroscopy , 1991 .

[25]  Timothy F. Havel,et al.  Ensemble quantum computing by NMR spectroscopy , 1997, Proc. Natl. Acad. Sci. USA.

[26]  Rafael Brüschweiler,et al.  One- and two-dimensional ensemble quantum computing in spin Liouville space , 1998 .

[27]  O. W. Sørensen A universal bound on spin dynamics , 1990 .