Dynamics of entanglement and state-space trajectories followed by a system of four-qubit in the presence of random telegraph noise: common environment (CE) versus independent environments (IEs)
Abstract:The paper investigates the dynamics of entanglement and explores some geometrical characteristics of the trajectories in state space, in four-qubit Greenberger-Horne-Zeilinger (GHZ) -and W-type states, coupled to common and independent classical random telegraph noise (RTN) sources. It is shown from numerical simulations that: (i) the dynamics of entanglement depends drastically not only on the input configuration of the qubits and the presence or absence of memory effects, but also on whether the qubits are c… Show more
“…The claim can be validated by looking at the previously studied various systems and situations where, preservation intervals are insignificant or less frequent. [ 20,21,24,35,36,55,56 ] We discovered that when Γ increases, the correlations between the qubits decrease. As the value of Γ increases, the curves shift from green to red causing a greater decay.…”
Section: Resultsmentioning
confidence: 99%
“…It is important to note that the final density matrices obtained for MMLR and NMLR given in Equations ( 14) and ( 15), both are completely different from those obtained for Gaussian and non-Gaussian noises studied in refs. [21,23,[35][36][37]43].…”
Section: Resultsmentioning
confidence: 99%
“…As seen by comparing previous results given in refs. [21,24,35,36,45,54,[57][58][59] to the current ones. Quantum correlations, coherence, and purity are all lost periodically when non-Markovian effects are maximized.…”
Section: Discussionmentioning
confidence: 99%
“…For instance, in the case of local channels, proper tuning of the noise phase and related parameters has been accomplished for optimal information preservation. [19][20][21] Besides all this, the local channels provide more degrees of freedom to analyze the dynamics of quantum systems. This will allow us to critically analyze the dynamical maps of the non-classical correlations versus the noise phase, related parameters, and system-environment coupling.…”
Section: Introductionmentioning
confidence: 99%
“…[20] Because of the RT noise, a variety of decay has been observed in bipartite, tripartite, multipartite and other hybrid quantum systems, where the systems become either separable or remain entangled under certain conditions given in refs. [21,[32][33][34][35][36][37]. From these references, we noticed the PWL noise causes a monotonic decay while the RT noise induces both exponential and oscillatory decay.…”
The collective effects of Markovian and non-Markovian classical fields on the dynamics of entanglement, coherence, and quantum state mixing in a three-qubit mixed entangled state are examined. Three independent local fields are considered to be influenced by the decoherence effects of two different mixed noisy models: Markovian maximized and non-Markovian maximized local random configurations. Power-law noise characterizes two classical environments in the first case, whereas random telegraph noise governs the third. Random telegraph noise rules two classical environments in the latter example, whereas power-law noise governs the third. In classical fields, non-Markovian effects are more robust and have a stronger character than Markovian effects, yet both are driven by relevant noises. Non-Markovianity vanishes at the upper bound of the Markovian noise parameters. Markovian effects are found to be vulnerable to the environments non-Markovianity and longer memory features. The strength of Markovianity and non-Markovianity is only moderately affected by the type of environment, but noise parameter optimization has a significant impact. Initial and final limits are provided for the restriction and relaxation in Markovianity and non-Markovianity of the classical fields for the actual deployment of non-local protocols.
“…The claim can be validated by looking at the previously studied various systems and situations where, preservation intervals are insignificant or less frequent. [ 20,21,24,35,36,55,56 ] We discovered that when Γ increases, the correlations between the qubits decrease. As the value of Γ increases, the curves shift from green to red causing a greater decay.…”
Section: Resultsmentioning
confidence: 99%
“…It is important to note that the final density matrices obtained for MMLR and NMLR given in Equations ( 14) and ( 15), both are completely different from those obtained for Gaussian and non-Gaussian noises studied in refs. [21,23,[35][36][37]43].…”
Section: Resultsmentioning
confidence: 99%
“…As seen by comparing previous results given in refs. [21,24,35,36,45,54,[57][58][59] to the current ones. Quantum correlations, coherence, and purity are all lost periodically when non-Markovian effects are maximized.…”
Section: Discussionmentioning
confidence: 99%
“…For instance, in the case of local channels, proper tuning of the noise phase and related parameters has been accomplished for optimal information preservation. [19][20][21] Besides all this, the local channels provide more degrees of freedom to analyze the dynamics of quantum systems. This will allow us to critically analyze the dynamical maps of the non-classical correlations versus the noise phase, related parameters, and system-environment coupling.…”
Section: Introductionmentioning
confidence: 99%
“…[20] Because of the RT noise, a variety of decay has been observed in bipartite, tripartite, multipartite and other hybrid quantum systems, where the systems become either separable or remain entangled under certain conditions given in refs. [21,[32][33][34][35][36][37]. From these references, we noticed the PWL noise causes a monotonic decay while the RT noise induces both exponential and oscillatory decay.…”
The collective effects of Markovian and non-Markovian classical fields on the dynamics of entanglement, coherence, and quantum state mixing in a three-qubit mixed entangled state are examined. Three independent local fields are considered to be influenced by the decoherence effects of two different mixed noisy models: Markovian maximized and non-Markovian maximized local random configurations. Power-law noise characterizes two classical environments in the first case, whereas random telegraph noise governs the third. Random telegraph noise rules two classical environments in the latter example, whereas power-law noise governs the third. In classical fields, non-Markovian effects are more robust and have a stronger character than Markovian effects, yet both are driven by relevant noises. Non-Markovianity vanishes at the upper bound of the Markovian noise parameters. Markovian effects are found to be vulnerable to the environments non-Markovianity and longer memory features. The strength of Markovianity and non-Markovianity is only moderately affected by the type of environment, but noise parameter optimization has a significant impact. Initial and final limits are provided for the restriction and relaxation in Markovianity and non-Markovianity of the classical fields for the actual deployment of non-local protocols.
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