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Nigerian Journal of Applied Physics

Simulation Of Quantum Spin Systems For Qubit Applications

Iyanuoluwa Olaniyi Ajayi

Published Sep 22, 2026• 0 citations
Publisher

Abstract

This study presents a numerical investigation of the dynamics of two coupled spin-1/2 quantum systems with emphasis on entanglement, quantum coherence, and state fidelity. The system is described by an isotropic Heisenberg Hamiltonian and investigated for exchange-coupling strengths J=−1, −0.5, 0, 0.5, and 11. Four representative initial states, comprising the Bell state, a partially entangled state with initial concurrence C (0) =0.8, and the separable states ∣01⟩and ∣++⟩are considered. Closed-system evolution is obtained using the unitary propagator, while environmental effects are modelled through a Lindblad master equation with local Markovian pure-dephasing channels for γ=0,0.1,0.5, and 11. The results show that the Bell state maintains maximal concurrence under closed Heisenberg evolution, while the partially entangled state retains its initial concurrence of 0.8 for all tested exchange couplings. In contrast, the initially separable ∣01⟩state develops strong transient entanglement through exchange interaction, reaching concurrence values essentially equal to unity for ∣J∣=0.5 and 11, whereas the ∣++⟩state remains separable to numerical precision. Under pure dephasing, concurrence and coherence decay progressively with increasing dephasing strength, while fidelity decreases toward its asymptotic value. The numerical calculations were further validated through normalization and Hermiticity checks, analytical dephasing benchmarks, and step-refinement convergence tests, with discrepancies remaining at machine-precision levels. The findings demonstrate that the preservation and generation of quantum correlations depend strongly on the initial state, exchange interaction, and environmental decoherence, providing validated numerical benchmarks for the study of coupled qubit dynamics.

DOI
10.62292/njap-v2i3-2026-94

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This study presents a numerical investigation of the dynamics of two coupled spin-1/2 quantum systems with emphasis on entanglement, quantum coherence, and state fidelity. The system is described by an isotropic Heisenberg Hamiltonian and investigated for exchange-coupling strengths J=−1, −0.5, 0, 0.5, and 11. Four representative initial states, comprising the Bell state, a partially entangled state with initial concurrence C (0) =0.8, and the separable states ∣01⟩and ∣++⟩are considered. Closed-system evolution is obtained using the unitary propagator, while environmental effects are modelled through a Lindblad master equation with local Markovian pure-dephasing channels for γ=0,0.1,0.5, and 11. The results show that the Bell state maintains maximal concurrence under closed Heisenberg evolution, while the partially entangled state retains its initial concurrence of 0.8 for all tested exchange couplings. In contrast, the initially separable ∣01⟩state develops strong transient entanglement through exchange interaction, reaching concurrence values essentially equal to unity for ∣J∣=0.5 and 11, whereas the ∣++⟩state remains separable to numerical precision. Under pure dephasing, concurrence and coherence decay progressively with increasing dephasing strength, while fidelity decreases toward its asymptotic value. The numerical calculations were further validated through normalization and Hermiticity checks, analytical dephasing benchmarks, and step-refinement convergence tests, with discrepancies remaining at machine-precision levels. The findings demonstrate that the preservation and generation of quantum correlations depend strongly on the initial state, exchange interaction, and environmental decoherence, providing validated numerical benchmarks for the study of coupled qubit dynamics.
The entanglement of two qubits, each defined as an effective two-level, spin 1/2 system, is investigated for the case that the qubits interact via a Heisenberg XY interaction and are subject to decoherence due to population relaxation and thermal effects. For zero temperature, the time-dependent concurrence is studied analytically and numerically for some typical initial states, including a separable (unentangled) initial state. An analytical formula for non-zero steady state concurrence is found for any initial state, and optimal parameter values for maximizing steady state concurrence are given. The steady state concurrence is found analytically to remain non-zero for low, finite temperatures. We also identify the contributions of global and local coherence to the steady state entanglement.
One of the main obstacles toward building efficient quantum computing systems is decoherence, where the inevitable interaction between the qubits and the surrounding environment leads to a vanishing entanglement. We consider a system of two interacting asymmetric two-level atoms (qubits) in the presence of pure and correlated dephasing environments. We study the dynamics of entanglement while varying the interaction strength between the two qubits, their relative frequencies, and their coupling strength to the environment starting from different initial states of practical interest. The impact of the asymmetry of the two qubits, reflected in their different frequencies and coupling strengths to the environment, varies significantly depending on the initial state of the system and its degree of anisotropy. For an initial disentangled, or a Werner, state, as the difference between the frequencies increases, the entanglement decay rate increases, with more persistence at the higher degrees of anisotropy in the former state. However, for an initial anti-correlated Bell state, the entanglement decays more rapidly in the symmetric case compared with the asymmetric one. The difference in the coupling strengths of the two qubits to the pure (uncorrelated) dephasing environment leads to higher entanglement decay in the different initial state cases, though the rate varies depending on the degree of anisotropy and the initial state. Interestingly, the correlated dephasing environment, within a certain range, was found to enhance the entanglement dynamics starting from certain initial states, such as the disentangled, anti-correlated Bell, and Werner, whereas it exhibits a decaying effect in other cases such as the initial correlated Bell state.
We theoretically consider the temporal dynamics of two coupled spin qubits (e.g., semiconductor quantum dots) driven by the interqubit spin-spin coupling. The presence of environmental noise (e.g., charge traps, nuclear spins, random magnetic impurities) is accounted for by including random magnetic field and random interqubit coupling terms in the Hamiltonian. Both Heisenberg coupling and Ising coupling between the spin qubits are considered, corresponding respectively to exchange and capacitive gates as appropriate for single spin and singlet-triplet semiconductor qubit systems, respectively. Both exchange (Heisenberg) and capacitive (Ising) coupling situations can be solved numerically exactly even in the presence of noise, leading to the key findings that (i) the steady-state return probability to the initial state remains close to unity in the presence of strong noise for many, but not all, starting spin configurations, and (ii) the return probability as a function of time is oscillatory with a characteristic noise-controlled decay toward the steady-state value. We also provide results for the magnetization dynamics of the coupled two-qubit system. Our predicted dynamics can be directly tested in the already existing semiconductor spin qubit setups providing insight into their coherent interaction dynamics. Retention of the initial state spin memory even in the presence of strong environmental noise has important implications for quantum computation using spin qubits.
The dynamics of two 1∕21∕21∕2-spin qubits under the influence of a quantum Heisenberg XYXYXY-type spin-bath is studied. After the Holstein-Primakoff transformation, numerical polynomial scheme is used to give the time-evolution calculation of the center qubits initially prepared in a product state or a Bell state. Then the concurrence of the two qubits, the zzz-component moment of either of the subsystem spins, and the fidelity of the subsystem are shown; they exhibit sensitive dependence on the anisotropic parameter, the temperature, the coupling strength, and the initial state. It is found that (i) the larger the anisotropic parameter $\ensuremath{\gamma}$, the bigger the probability of maintaining the initial state of the two qubits; (ii) with increasing temperature TTT, the bath plays a stronger destroy effect on the dynamics of the subsystem, so does the interaction g0{g}_{0}g0​ between the subsystem and the bath; and (iii) the time evolution of the subsystem is dependent on the initial state. The revival of the concurrence does not always mean the restoration of the state. Further, the dynamical properties of the subsystem should be judged by the combination of concurrence and fidelity.
The decoherence and entanglement dynamics of two interacting qubits coupled through Heisenberg XY interactions to a spin bath in thermal equilibrium are studied. The exact form of the reduced density matrix is derived for finite and infinite numbers of environmental spins. It is shown that decoherence can be minimized at low bath temperatures and strong coupling between the qubits. Some initial product states evolve into entangled ones, initially entangled states lose completely or partially their entanglement. The relation between the fidelity and the concurrence is also investigated.
The dynamics of entanglement and fidelity for a subsystem of two separate spin-1∕21∕21∕2 qubits prepared in Bell states is investigated. One of the subsystem qubit labeled AAA is under the influence of a Heisenberg XYXYXY spin bath, while another one labeled BBB is uncoupled with that. We discuss two cases: (i) the number of bath spins is infinite, $N\ensuremath{\rightarrow}\ensuremath{\infty}$, and (ii) NNN is finite, N=40N=40N=40. In both cases, the bath is initially prepared in a thermal equilibrium state. It is shown that the time dependence of the concurrence and the fidelity of the two subsystem qubits can be controlled by tuning the parameters of the spin bath, such as the anisotropic parameter, the temperature, and the coupling strength with qubit AAA. It is interesting to find that the dynamics of the concurrence is independent of four different initial Bell states and that of the fidelity is divided into two groups.