-
1
-
-
0029388979
-
-
For reviews, see D.P. DiVincenzo, Science 270, 255 (1995);
-
(1995)
Science
, vol.270
, pp. 255
-
-
DiVincenzo, D.P.1
-
5
-
-
0003504974
-
-
B.S. DeWitt, R. Stora, North-Holland, Amsterdam
-
R. Jackiw, in Relativity Groups and Topology, Les Houches 1983, edited by B.S. DeWitt and R. Stora (North-Holland, Amsterdam, 1984), p. 154.
-
(1984)
Relativity Groups and Topology, Les Houches 1983
, pp. 154
-
-
Jackiw, R.1
-
6
-
-
85035300960
-
-
For a review see, Geometric Phases in Physics, edited by A. Shapere and F. Wilczek (World Scientific, Singapore, 1989)
-
For a review see, Geometric Phases in Physics, edited by A. Shapere and F. Wilczek (World Scientific, Singapore, 1989).
-
-
-
-
7
-
-
85035290599
-
-
A. Kitaev, e-print archive quant-ph/9707021.
-
-
-
Kitaev, A.1
-
8
-
-
0003482738
-
-
S. Popescu, T. Spiller, World Scientific, Singapore
-
J. Preskill, in Introduction to Quantum Computation and Information, edited by S. Popescu, and T. Spiller, Hoi-Kwong Lo (World Scientific, Singapore, 1999).
-
(1999)
Introduction to Quantum Computation and Information
-
-
Preskill, J.1
-
11
-
-
85035298056
-
-
We thank H. Barnum for pointing out this possibility
-
We thank H. Barnum for pointing out this possibility.
-
-
-
-
12
-
-
85035294216
-
-
The notation (Formula presented) means that X has nontrivial action only on the (Formula presented)th factor of (Formula presented)
-
The notation (Formula presented) means that X has nontrivial action only on the (Formula presented)th factor of (Formula presented).
-
-
-
-
13
-
-
85035294130
-
-
When the system geometry is given, one can restrict to “local” gates without loss of efficiency
-
When the system geometry is given, one can restrict to “local” gates without loss of efficiency.
-
-
-
-
14
-
-
0001335519
-
-
D. Deutsch, A. Barenco, and A. Ekert, Proc. R. Soc. London, Ser. A 449, 669 (1995);
-
(1995)
Proc. R. Soc. London, Ser. A
, vol.449
, pp. 669
-
-
Deutsch, D.1
Barenco, A.2
Ekert, A.3
-
16
-
-
85035285170
-
-
For example, one could consider N qu-trits, i.e., (Formula presented) such that (Formula presented) admits a four-dimensional degenerate eigenspace (Formula presented). Assuming for the (Formula presented)’s the conditions stated in the text, HQC can be efficiently implemented over (Formula presented). Notice that in this case the dimension of the physical state space is increased (Formula presented) instead of (Formula presented)
-
For example, one could consider N qu-trits, i.e., (Formula presented) such that (Formula presented) admits a four-dimensional degenerate eigenspace (Formula presented). Assuming for the (Formula presented)’s the conditions stated in the text, HQC can be efficiently implemented over (Formula presented). Notice that in this case the dimension of the physical state space is increased (Formula presented) instead of (Formula presented).
-
-
-
|