Abstract

The interacting of two qubits and an N-level atom based on su(2) Lie algebra in the presence of both qubit–qubit interaction and dissipation term is considered. The effects of the qubit–qubit interaction and the dissipation term on the dynamics of the proposed system are discussed in detail for certain values of the number of levels. The dynamical expressions of the observable operators are obtained using the Heisenberg equation of motion. The population inversion and linear entropy, as well as the concurrence formula as a measure of entanglement between the two qubits are calculated and discussed. The roles of the number of levels, the qubit–qubit coupling parameter and the dissipation rate on these quantities are also discussed. We explore the sudden birth and sudden death of the entanglement phenomena with and without the dissipation term.

Highlights

  • The interacting of two qubits and an N-level atom based on su(2) Lie algebra in the presence of both qubit–qubit interaction and dissipation term is considered

  • The phenomena of entanglement sudden death (ESD) and entanglement sudden birth (ESB) were found to depend on the kind of time-dependent coupling between the two a­ toms[23]

  • It is shown that the occurrence of sudden death and sudden birth phenomena can be controlled by the coupling phase parameter

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Summary

Description of the model and solution

An application of the su(2) algebraic system has been presented ­in[31,32] They examined the star network of spins, where all rotations interact exclusively and continuously with a central rotation through Heisenberg XX couplings of equal strength. K=1 where γ denotes the decay rate, J− , J+ denote the lowering and raising operators of the su(2) symmetry and satisfy the following commutation relation:. =i (S112J− − S211J+) + i (S122J− − S221J+), dS1k1 = − i dt (S1k2J− − S2k1J+) + R. k=1 where Cis a constant of motion. The general solution for the two-qubit is obtained by calculating the time evolution operator as follows,. Under the the analytical exact form orefstohneatnimceeceavsoelcuotniodnitoiopner(aδtz1o+r Uδ2z(=t)0is) and for space given by of the two qubits as. After obtained on the wave function (15) can be used to describe the evolution of some quantum quantifiers as: population inversion, linear entropy and concurrence

Population inversion
Linear entropy
Linear Entropy
Conclusion
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