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1
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Knill, E.1
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84894388797
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note
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The controlled-Z gate is represented by the matrix (1 0 0 0) (0 1 0 0) (0 0 1 0) (0 0 0 -1) This gate changes the state + 11> to - 11> and leaves the states 00>, 01>, and unchanged.
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4
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33744535413
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"Cluster-state quantum computation"
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M. A. Nielsen, "Cluster-state quantum computation," Rep. Math. Phys. 57, 147-161 (2006).
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Nielsen, M.A.1
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Browne, D.E.1
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6
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"Experimental one-way quantum computing"
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P. Walther, K. J. Resch, T. E. Rudolph, E. Schenck, H. Weinfurter, V. Vedral, M. Aspelmeyer, and A. Zeilinger, "Experimental one-way quantum computing," Nature 434, 169-176 (2005).
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Vedral, V.6
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Zeilinger, A.8
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7
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33144461649
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"Experimental construction of optical multiqubit cluster states from Bell states"
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A. N. Zhang, C. Y. Lu, X. Q. Zhou, Y. A. Chen, Z. Zhao, T. Yang, and J. W. Pan, "Experimental construction of optical multiqubit cluster states from Bell states," Phys. Rev. A 73, 022330 (2006).
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8
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0032621435
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"Pulsed energy-time entangled twin-photon source for quantum communication"
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9
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19744382431
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"Distribution of time bin entangled qubits over 50 km of optical fiber"
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I. Marcikie, H. de Riedmatten, W. Tittel, H. Zbinden, M. Legré, and N. Gisin, "Distribution of time bin entangled qubits over 50 km of optical fiber," Phys. Rev. Lett. 93, 180502 (2004).
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11
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in (IEEE), paper TuB3.1
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Bussières, F.1
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12
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84894388363
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note
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-iφ sin(θ) cos(θ)), where cos(θ) equals the reflectivity of the beam splitter. The notation "50:50 beamsplitter" used in this paper corresponds to θ=45° and φ=0.
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13
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84894388829
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note
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iθ/2), which is equivalent to applying the phase -θ/2 to state 0) and phase + 0/2 to state 1>.
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