Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

MAXENT APPROACH TO QUBITS

Claudia M. Sarris, Araceli N. Proto, F. Bary Malik

Published Sep 1, 2007• 0 citations
Publisher
DOI
10.1142/9789812709592_0041

Related papers

QUANTUM MECHANICS OF QUBITS

WORLD SCIENTIFIC eBooks•Jul 21, 2019•0 citations

BLACK HOLES AND QUBITS

L. Borsten, M. J. Duff, W. Rubens

•Jul 16, 2012•1 citation

QUBITS

McGill-Queen's University Press eBooks•Apr 2, 2024•0 citations

TALKING BREATHER QUBITS

Toshiyuki Fujii, Munehiro Nishida, Satoshi Tanda +1 more

•Dec 1, 2009•0 citations

Computation with Qubits

WORLD SCIENTIFIC eBooks•Jul 15, 2020•0 citations

MAXENT APPROACH TO QUBITS

Claudia M. Sarris, Araceli N. Proto, F. Bary Malik

We consider the Hubbard-like Hamiltonian used in Physica B 352 (2004) 269-279, using the MaxEnt approach and a CSCO, as the set of relevant operators which, obviously, close a partial Lie algebra with the Hamiltonian. So, it is possible to define a positive definite metric on the space spanned by the mean values of the CSCO. Particularly, the selected operators represent the occupation number, the aligned and antialigned pairs per site, respectively. The interesting question to be examined here is whether the above mentioned Hamiltonian have the property that the expectation values of a suitable operator are indeed zero and one (or a constant) qubits, and zero and +1 and -1, i.e., qutrits.

International Journal of Modern Physics B•May 30, 2007•1 citation
We consider the Hubbard-like Hamiltonian used in Physica B 352 (2004) 269-279, using the MaxEnt approach and a CSCO, as the set of relevant operators which, obviously, close a partial Lie algebra with the Hamiltonian. So, it is possible to define a positive definite metric on the space spanned by the mean values of the CSCO. Particularly, the selected operators represent the occupation number, the aligned and antialigned pairs per site, respectively. The interesting question to be examined here is whether the above mentioned Hamiltonian have the property that the expectation values of a suitable operator are indeed zero and one (or a constant) qubits, and zero and +1 and -1, i.e., qutrits.