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1
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0029388979
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For reviews, see D.P. DiVincenzo, Science 270, 255 (1995)
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(1995)
Science
, vol.270
, pp. 255
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DiVincenzo, D.P.1
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3
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85037189898
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The set of operators over (Formula presented) is endowed with the Hilbert space topology generated by the Hilbert-Schmidt scalar product (Formula presented)
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The set of operators over (Formula presented) is endowed with the Hilbert space topology generated by the Hilbert-Schmidt scalar product (Formula presented).
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5
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0001335519
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D. Deutsch, A. Barenco, and A. Ekert, Proc. R. Soc. London, Ser. A 449, 669 (1995)
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(1995)
Proc. R. Soc. London, Ser. A
, vol.449
, pp. 669
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Deutsch, D.1
Barenco, A.2
Ekert, A.3
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12
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85037187563
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Let (Formula presented) be the group generated by the (Formula presented)’s (Formula presented)’s]. (Formula presented) is an algebra isomorphism; then (Formula presented) Moreover, from continuity, (Formula presented)
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Let (Formula presented) be the group generated by the (Formula presented)’s (Formula presented)’s]. (Formula presented) is an algebra isomorphism; then (Formula presented) Moreover, from continuity, (Formula presented).
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13
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85037210085
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Phys. Lett. (to be published)
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P. Zanardi, Phys. Lett. (to be published).
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Zanardi, P.1
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15
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85037225047
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J.F. Cornwell, Group Theory in Physics (Academic, New York, 1984), Vol. I–III
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J.F. Cornwell, Group Theory in Physics (Academic, New York, 1984), Vol. I–III.
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16
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85037227172
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Let (Formula presented) be a basis of (Formula presented); then (Formula presented) is defined as the linear space of (formal) polynomials in the (Formula presented)’s. The latter satisfy the relations (Formula presented) where (Formula presented) are the structure constants of (Formula presented), and (Formula presented)
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Let (Formula presented) be a basis of (Formula presented); then (Formula presented) is defined as the linear space of (formal) polynomials in the (Formula presented)’s. The latter satisfy the relations (Formula presented) where (Formula presented) are the structure constants of (Formula presented), and (Formula presented).
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17
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85037182684
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Given a group (Formula presented) of finite order, its group algebra (Formula presented) is the vector space generated by complex combinations of elements of (Formula presented). Multiplication is introduced by linear extension of the group operation
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Given a group (Formula presented) of finite order, its group algebra (Formula presented) is the vector space generated by complex combinations of elements of (Formula presented). Multiplication is introduced by linear extension of the group operation.
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18
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85037215920
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Using this expression one can easily check that the equation (Formula presented), following immediately from Eq. (3), reproduces the correct Catalan numbers (Formula presented)
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Using this expression one can easily check that the equation (Formula presented), following immediately from Eq. (3), reproduces the correct Catalan numbers (Formula presented).
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20
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85037253312
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Indeed, if (Formula presented) and (Formula presented), one has (Formula presented) in that (Formula presented). Conversely, suppose (Formula presented) and (Formula presented) The elements of the one-parameter subgroup generated by y, (Formula presented), satisfy (Formula presented); then (Formula presented)
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Indeed, if (Formula presented) and (Formula presented), one has (Formula presented) in that (Formula presented). Conversely, suppose (Formula presented) and (Formula presented) The elements of the one-parameter subgroup generated by y, (Formula presented), satisfy (Formula presented); then (Formula presented).
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21
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85037213922
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E. Knill LANL, e-print archive quant-ph/9608048.
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Knill, E.1
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23
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26144467285
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W.M. Itano, D.J. Heinzen, D.J. Bollinger, and D.J. Wineland, Phys. Rev. A 41, 2295 (1990).
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(1990)
Phys. Rev. A
, vol.41
, pp. 2295
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Itano, W.M.1
Heinzen, D.J.2
Bollinger, D.J.3
Wineland, D.J.4
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