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Physica D Nonlinear Phenomena

Fractional Schrödinger dynamics and decoherence

Kay Kirkpatrick, Yanzhi Zhang

Published Jun 27, 2016• 51 citations
Publisher
DOI
10.1016/j.physd.2016.05.015

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This is a novel approach to mitigating decoherence in quantum computing with "Fractional-Time Qubits: Leveraging Memory Kernels to Combat Decoherence in Quantum Computing." In this work, Erika Barker introduces fractional quantum dynamics by replacing the conventional time derivative in Schrödinger’s equation with a fractional derivative of order β. This modification incorporates long-range memory kernels—crucial for modeling 1/f noise and other non-Markovian effects—that fundamentally alter decoherence profiles and extend qubit lifetimes. Key highlights include: Expanded Hilbert Space Formalism: A novel framework that embeds fractional dynamics into a larger, unitary space, ensuring probability conservation and a generalized energy conservation law reminiscent of pseudo-Hermitian quantum mechanics. Noise Mitigation Strategies: Detailed analysis and numerical simulations demonstrate how fractional dynamics produce stretched-exponential and power-law decays, effectively countering decoherence in 1/f, Ohmic, and sub-Ohmic noise environments. Resource Efficiency: A comparative discussion on resource overhead reveals potential advantages over traditional quantum error correction, offering a promising pathway for near-term quantum devices with limited qubit counts. Interdisciplinary Impact: The paper also connects these techniques with broader theoretical frameworks in quantum gravity and fractal time, suggesting far-reaching implications for both practical quantum engineering and fundamental physics. This comprehensive study provides essential insights for researchers focused on quantum decoherence, advanced error mitigation techniques, and the development of robust quantum computing architectures. Keywords: quantum computing, decoherence, fractional dynamics, memory kernels, 1/f noise, non-Markovian, Hilbert space, quantum error correction.

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The Time-Fractional Schrödinger Equation (TFSE) is an effective tool for simulating the dynamics of non-Markovian quantum systems. The Quantum Speed Limit (QSL) time characterizes the minimum time required for the evolution of a non-Markovian quantum system. In this paper, Wei's TFSE is employed to simulate the non-Markovian quantum accelerated evolution process in the Resonant Dissipative Jaynes-Cummings (RDJC) model. By solving the QSL time of a time-fractional single-qubit open system, the enhancement mechanism of the system evolution speed induced by the non-Markovian memory effects of the environment is revealed. Further studies show that the optimized acceleration of the system evolution can be achieved by jointly regulating the fractional order, coupling strength, and photon number. Comparative analyses indicate that Wei's TFSE can accurately capture the non-Markovian accelerated dynamical features of the system over the entire fractional order range, whereas Naber's TFSE is applicable only within a limited fractional order interval. In addition, the comparisons of the average simulation time for calculating the dynamical trajectory of the excited-state probability demonstrate that Wei's TFSE has a significant simulation advantage in computational efficiency. Therefore, Wei's TFSE is more accurate and efficient for simulating the accelerated dynamics of non-Markovian quantum systems.

quant-pharXiv:2606.20024•Jun 19, 2026•0 citations
This is a novel approach to mitigating decoherence in quantum computing with "Fractional-Time Qubits: Leveraging Memory Kernels to Combat Decoherence in Quantum Computing." In this work, Erika Barker introduces fractional quantum dynamics by replacing the conventional time derivative in Schrödinger’s equation with a fractional derivative of order β. This modification incorporates long-range memory kernels—crucial for modeling 1/f noise and other non-Markovian effects—that fundamentally alter decoherence profiles and extend qubit lifetimes. Key highlights include: Expanded Hilbert Space Formalism: A novel framework that embeds fractional dynamics into a larger, unitary space, ensuring probability conservation and a generalized energy conservation law reminiscent of pseudo-Hermitian quantum mechanics. Noise Mitigation Strategies: Detailed analysis and numerical simulations demonstrate how fractional dynamics produce stretched-exponential and power-law decays, effectively countering decoherence in 1/f, Ohmic, and sub-Ohmic noise environments. Resource Efficiency: A comparative discussion on resource overhead reveals potential advantages over traditional quantum error correction, offering a promising pathway for near-term quantum devices with limited qubit counts. Interdisciplinary Impact: The paper also connects these techniques with broader theoretical frameworks in quantum gravity and fractal time, suggesting far-reaching implications for both practical quantum engineering and fundamental physics. This comprehensive study provides essential insights for researchers focused on quantum decoherence, advanced error mitigation techniques, and the development of robust quantum computing architectures. Keywords: quantum computing, decoherence, fractional dynamics, memory kernels, 1/f noise, non-Markovian, Hilbert space, quantum error correction.
In this paper, we examine the time-fractional Schrödinger equation from the perspective of non-Markovian dynamics in dissipative systems. First, we determine the range of the fractional derivative's order by examining the memory properties of the time-fractional Schrödinger equation. Next, we employ the Jaynes-Cummings model to identify the appropriate mathematical form of the imaginary unit. Finally, we use the refined equation to study quantum teleportation under amplitude damping noise. It was found that the time-fractional Schrödinger equation without fractional operations on the imaginary unit i might be more suitable for describing non-Markovian dynamics in dissipative systems. Our research may provide a new perspective on the time-fractional Schrödinger equation, contributing to a deeper understanding and further development of time-fractional quantum mechanics.
The Time-Fractional Schrödinger Equation (TFSE) is an effective tool for simulating the dynamics of non-Markovian quantum systems. The Quantum Speed Limit (QSL) time characterizes the minimum time required for the evolution of a non-Markovian quantum system. In this paper, Wei's TFSE is employed to simulate the non-Markovian quantum accelerated evolution process in the Resonant Dissipative Jaynes-Cummings (RDJC) model. By solving the QSL time of a time-fractional single-qubit open system, the enhancement mechanism of the system evolution speed induced by the non-Markovian memory effects of the environment is revealed. Further studies show that the optimized acceleration of the system evolution can be achieved by jointly regulating the fractional order, coupling strength, and photon number. Comparative analyses indicate that Wei's TFSE can accurately capture the non-Markovian accelerated dynamical features of the system over the entire fractional order range, whereas Naber's TFSE is applicable only within a limited fractional order interval. In addition, the comparisons of the average simulation time for calculating the dynamical trajectory of the excited-state probability demonstrate that Wei's TFSE has a significant simulation advantage in computational efficiency. Therefore, Wei's TFSE is more accurate and efficient for simulating the accelerated dynamics of non-Markovian quantum systems.