M. A. Rowe, A. Ben-Kish, B. DeMarco, D. Leibfried, V. Meyer, J. Beall, J. Britton, J. Hughes, W. M. Itano, B. Jelenković, et al., Quant. Inf. Comp. 2
2002
Cited alongside, same era.
C. M. Tesch and R. de Vivie-Riedle, Phys. Rev. Lett. 89
2002
Cited alongside, same era.
F. Schmidt-Kaler, H. Häffner, S. Gulde, M. Riebe, G. P. T. Lancaster, T. Deuschle, C. Becher, W. Hänsel, J. Eschner, C. F. Roos, et al., Appl. Phys. B 77
2003
Cited alongside, same era.
D. Leibfried, B. DeMarco, V. Meyer, D. Lucas, M. Barrett, J. Britton, W. M. Itano, B. Jelenković, C. Langer, T. Rosenband, et al., Nature 422
2003
Cited alongside, same era.
J. P. Palao and R. Kosloff, Phys. Rev. A 68
2003
Cited alongside, same era.
L. M. K. Vandersypen and I. L. Chuang, Rev. Mod. Phys. 76
2004
Cited alongside, same era.
J. Chiaverini, D. Leibfried, T. Schaetz, M. D. Barrett, R. B. Blakestad, J. Britton, W. M. Itano, J. D. Jost, E. Knill, C. Langer, et al., Nature 432
2004
Cited alongside, same era.
N. Khaneja, T. Reiss, C. Kehlet, T. Schulte-Herbrüggen, and S. J. Glaser, J. Magn. Reson. 172
2005
Cited alongside, same era.
Assuming that a single-qubit gate is performed with a laser beam with intensity I I and a Gaussian spatial beam profile with waist w w , it is advantageous to work with an interaction whose strengths falls off as θ ( r ) ∝ exp ( − 2 r 2 / w 2 ) \theta(r)\propto\exp(-2r^{2}/w^{2}) instead of θ ( r ) ∝ I ∝ exp ( − r 2 / w 2 ) \theta(r)\propto\sqrt{I}\propto\exp(-r^{2}/w^{2})
Cited in the paper.
If the sum in eq. ( 2
Cited in the paper.
As the Hamiltonians in set 𝒮 \cal S are sufficient for generating arbitrary unitary operations, we did not include the Hamiltonians S Y S_{Y} , S Y 2 S_{Y}^{2} . However, as these Hamiltonians are experimentally as easily generated as S X S_{X} , S X 2 S_{X}^{2} by shifting the optical phase of the control laser field by π / 2 \pi/2 with the help of an acousto-optical modulator, we use them in some of the pulse sequences for constructing the desired target operation
Cited in the paper.