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

$SU(N)$ Fidelity and Maximally Entangled States of Qubit and Qutrit Bipartite Systems

Surajit Sen, T.K. Dey

Published Nov 9, 2019• 0 citations
OpenAlex

Related papers

Maximally entangled states for qubit- qutrit systems

Mohsen Sarbishaei

Indian Journal of Physics•Mar 12, 2005•0 citations

SU(N) algebras and new thumbrules for entanglement of bipartite qubit and qutrit systems

P. Dasgupta, Debashis Gangopadhyay

Based on the Schmidt decomposition new convenient thumbrules are obtained to test entanglement of wavefunctions for bipartite qubit and qutrit systems. For the qubit system there is an underlying SU(2) algebra , while the same for a qutrit system is SU(3).

arXiv:2408.02702•Aug 4, 2024•0 citations

Teleportation with non-maximally entangled states and underlying unitary algebras of certain bipartite systems

P. Dasgupta, Debashis Gangopadhyay

New convenient thumbrules are obtained to test entanglement of wavefunctions for bipartite qubit and qutrit systems. All results are analytic. The new results are: (a) For bipartite qubit systems there exists a matrix $A$ for which $\det A = 0$ implies unentanglement while $\det A \ne 0$ implies entanglement. There is an underlying SU(2) algebra. (2) Teleportation for a general qubit state is possible by using non-maximally entangled bipartite qubit states. This protocol has an additional parameter, viz., $\det A$, which enhances the cryptographic security of the teleportation. (c) For qutrits there is a matrix $P$ for which $\det P = 0$ simultaneously with ${\rm tr}P=\pm 1$ imply unentanglement. Any departure from these conditions implies entanglement. There exists an underlying SU(3) algebra. (d) Physical interpretation of the underlying algebras are given and plausible experimental scenarios are proposed for the SU(2) case in the context of two entangled electrons. (e) The entanglement entropy in both cases, viz., for qubits and qutrits respectively, are expressed in terms of the determinants and trace of the matrices mentioned above.

arXiv:2505.21084•May 27, 2025•0 citations

Maximal entanglement of bipartite spin states in the context of quantum algebra

K. Berrada, Y. Hassouni

The European Physical Journal D•Dec 3, 2010•24 citations

Entangled States of Qutrit Bipartite System

Surajit Sen, Dey, Tushar Kanti

We develop a systematic method to construct the Bell states of a qubit bipartite system while taking $SU(2)$ group as the basis group. An alternative formulation of fidelity, called $SU(2)$ fidelity, is proposed which gives the Bell-CHSH inequality. Taking analogy from the octet theory governed by the $SU(3)$ group, it is shown that the method can be easily generalized to derive all possible entangled states and the $SU(3)$ fidelity of the higher dimensional bipartite qutrit system. The properties of these states are studied which reveal the existence of some inequalities for the qutrit bipartite system.

arXiv:1911.03628•Nov 9, 2019•0 citations

Beyond the Entanglement of Qubit Pairs in Multipartite Systems

S. Shelly Sharma, Naresh Kumar Sharma

•Jan 1, 2022•1 citation
SU(N)SU(N)SU(N) Fidelity and Maximally Entangled States of Qubit and Qutrit Bipartite Systems
New convenient thumbrules are obtained to test entanglement of wavefunctions for bipartite qubit and qutrit systems. All results are analytic. The new results are: (a) For bipartite qubit systems there exists a matrix AAA for which det⁡A=0\det A = 0detA=0 implies unentanglement while det⁡A≠0\det A \ne 0detA=0 implies entanglement. There is an underlying SU(2) algebra. (2) Teleportation for a general qubit state is possible by using non-maximally entangled bipartite qubit states. This protocol has an additional parameter, viz., det⁡A\det AdetA, which enhances the cryptographic security of the teleportation. (c) For qutrits there is a matrix PPP for which det⁡P=0\det P = 0detP=0 simultaneously with trP=±1{\rm tr}P=\pm 1trP=±1 imply unentanglement. Any departure from these conditions implies entanglement. There exists an underlying SU(3) algebra. (d) Physical interpretation of the underlying algebras are given and plausible experimental scenarios are proposed for the SU(2) case in the context of two entangled electrons. (e) The entanglement entropy in both cases, viz., for qubits and qutrits respectively, are expressed in terms of the determinants and trace of the matrices mentioned above.
We develop a systematic method to construct the Bell states of a qubit bipartite system while taking SU(2)SU(2)SU(2) group as the basis group. An alternative formulation of fidelity, called SU(2)SU(2)SU(2) fidelity, is proposed which gives the Bell-CHSH inequality. Taking analogy from the octet theory governed by the SU(3)SU(3)SU(3) group, it is shown that the method can be easily generalized to derive all possible entangled states and the SU(3)SU(3)SU(3) fidelity of the higher dimensional bipartite qutrit system. The properties of these states are studied which reveal the existence of some inequalities for the qutrit bipartite system.