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Physical review. B, Condensed matter

Analysis of Landau-Zener tunneling with an Ohmic reservoir and a noise source

Tatsuya Usuki

Published Mar 15, 1998• 7 citations
Publisher

Abstract

To determine the possibility of single-electron operation in electronic devices, we investigated the Landau-Zener (LZ) tunneling process with dissipation. This work presents an analytical formula and detailed numerical results for dynamical tunneling phenomena with an Ohmic reservoir and a noise source. First, we calculated the transient and final density matrices of a single-electron system coupled to a reservoir at zero temperature, and then noted the rigid tunneling process and a noticeable decoherence of the tunneling. The rigidity of the LZ tunneling suggests that we can suppress errors in single-electron operations. However, our analytical and numerical results clarified the fact that noise strongly affects the tunneling process. When half of the noise spectrum bandwidth ${\ensuremath{\omega}}_{\mathrm{max}}$ is larger than the gap of the adiabatic potential, thermal excitation by the noise source considerably increases the tunneling probability. On the other hand, our numerical results found that the noise effect is proportional to ${\ensuremath{\omega}}_{\mathrm{max}}^{3}$ when ${\ensuremath{\omega}}_{\mathrm{max}}$ is smaller than the gap. Then we can accurately operate single electrons if the noise source has a sufficiently narrow band.

DOI
10.1103/physrevb.57.7124

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To determine the possibility of single-electron operation in electronic devices, we investigated the Landau-Zener (LZ) tunneling process with dissipation. This work presents an analytical formula and detailed numerical results for dynamical tunneling phenomena with an Ohmic reservoir and a noise source. First, we calculated the transient and final density matrices of a single-electron system coupled to a reservoir at zero temperature, and then noted the rigid tunneling process and a noticeable decoherence of the tunneling. The rigidity of the LZ tunneling suggests that we can suppress errors in single-electron operations. However, our analytical and numerical results clarified the fact that noise strongly affects the tunneling process. When half of the noise spectrum bandwidth \ensuremathωmax{\ensuremath{\omega}}_{\mathrm{max}}\ensuremathωmax​ is larger than the gap of the adiabatic potential, thermal excitation by the noise source considerably increases the tunneling probability. On the other hand, our numerical results found that the noise effect is proportional to \ensuremathωmax3{\ensuremath{\omega}}_{\mathrm{max}}^{3}\ensuremathωmax3​ when \ensuremathωmax{\ensuremath{\omega}}_{\mathrm{max}}\ensuremathωmax​ is smaller than the gap. Then we can accurately operate single electrons if the noise source has a sufficiently narrow band.
In this work, we investigate the influence of colored noise originating from a heat bath on nonlinear Landau-Zener (LZ) tunneling. The nonlinearity might arise intrinsically from many-body mean-field atomic self-interactions or Kerr nonlinearities in optical systems. Contrary to the well-established picture of thermally enhanced quantum tunneling within the linear LZ paradigm, ensemble statistics of our numerical simulations demonstrate that nonlinearity can give rise to thermally suppressed LZ tunneling: the tunneling probability of the nonlinear LZ system decreases as the amplitude of the colored noise increases beyond a critical value. Analytically, the Wiener-Hermite expansion facilitates elucidation of the intrinsic mechanism accounting for the nonmonotonic dependence of tunneling probability on noise amplitude. We compare these behaviors with stochastic resonance responses and clarify that the two phenomena stem from distinct physical mechanisms. In addition, we obtain approximate solutions in the weak- and strong-noise limits and discuss the implications of our theory.
We determine the Landau-Zener transition probability in a dissipative environment including both longitudinal as well as transversal quantum-mechanical noise originating from a single noise source. For this, we use the numerically exact quasiadiabatic path integral, as well as the approximative nonequilibrium Bloch equations. We find that transversal quantum noise in general influences the Landau-Zener probability much more strongly than longitudinal quantum noise does at a given temperature and system-bath coupling strength. In other words, transversal noise contributions become important even when the coupling strength of transversal noise is smaller than that of longitudinal noise. We furthermore reveal that transversal noise renormalizes the tunnel coupling independent of temperature. Finally, we show that the effect of mixed longitudinal and transversal noise originating from a single bath cannot be obtained from an incoherent sum of purely longitudinal and purely transversal noise.
The quantum dynamics of the Landau-Zener transition in a dissipative environment is studied and analytical results for the transition probability are given in terms of temperature, coupling strength, and the Landau-Zener time. For short Landau-Zener time there is no effect of dissipation. In the oppotise limit we distinguish various temperature regimes: The adiabatic limit is shown to be restricted to low temperatures and no effect of dissipation is present at zero temperature. At intermediate temperatures thermal transitions dominate for weak coupling and high temperatures correspond to the strong-coupling limit.
Long-distance transfer of quantum information in architectures based on quantum dot spin qubits will be necessary for their scalability. One way of achieving this goal is to simply move the electron between two quantum registers. Precise control over the process of shuttling such a single electron through a chain of tunnel-coupled quantum dots is possible when interdot energy detunings are changed adiabatically. The deterministic character of shuttling is, however, endangered by the open nature of the system, as the transferred electron is coupled to thermal reservoirs: sources of fluctuations of electric fields and lattice vibrations. We present a comprehensive analysis showing how the electron transfer between two voltage-controlled quantum dots is affected by electron-phonon scattering and interaction with sources of 1/f1/f1/f and Johnson charge noise in both detuning and tunnel coupling. The electron-phonon scattering turns out to be irrelevant in Si quantum dots, with charge noise dominating the dynamics of the system at slow detuning sweep, when the electron spends more time delocalized between the dots (i.e., near the anticrossing of the tunnel-coupled states). Competition between the effects of charge noise and the Landau-Zener effect leads to an existence of an optimal detuning sweep rate, leading to minimal probability of leaving the electron behind. In GaAs quantum dots, on the other hand, piezoelectric coupling to phonons is strong enough to make the processes of interdot transfer assisted by phonon emission and absorption dominate over transitions caused by charge noise. The probability of leaving the electron behind then depends monotonically on detuning the sweep rate over a broad range of rates, and values much smaller than in silicon can be obtained for slow sweeps. However, after taking into account limitations on transfer time imposed by the need for preservation of a shuttled electron's spin coherence, the minimal probabilities of leaving the electron behind in both GaAs- and Si-based double quantum dots turn out to be of the same order of magnitude. Bringing them down below ${10}^{\ensuremath{-}3}$ requires temperatures $\ensuremath{\le}100$ mK and tunnel couplings above $20\phantom{\rule{4pt}{0ex}}\ensuremath{\mu}\mathrm{eV}$.
We investigate the influence of temperature and dissipation on the Landau–Zener transition probability in circuit QED. Dissipation is modelled by coupling the transmission line to a bath of harmonic oscillators, and the reduced density operator is treated within Bloch–Redfield theory. A phase-space representation allows an efficient numerical implementation of the resulting master equation. It provides reliable results which are valid even for rather low temperatures. We find that the spin-flip probability as a function of temperature and dissipation strength exhibits a non-monotonic behaviour. Our numerical results are complemented by analytical solutions for zero temperature and for vanishing dissipation strength.
We investigate the influence of temperature and dissipation on the Landau–Zener transition probability in circuit QED. Dissipation is modelled by coupling the transmission line to a bath of harmonic oscillators, and the reduced density operator is treated within Bloch–Redfield theory. A phase-space representation allows an efficient numerical implementation of the resulting master equation. It provides reliable results which are valid even for rather low temperatures. We find that the spin-flip probability as a function of temperature and dissipation strength exhibits a non-monotonic behaviour. Our numerical results are complemented by analytical solutions for zero temperature and for vanishing dissipation strength.