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Optics Communications

Geometric phase for a coupled two quantum dot system

Amitabh Joshi, Shoukry S. Hassan

Published Feb 22, 2011• 2 citations
Publisher
DOI
10.1016/j.optcom.2011.01.066

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We study theoretically the geometric phase of a double-quantum-dot (DQD) system measured by a quantum point contact (QPC) in the pure dephasing and dissipative environments, respectively. The results show that in these two environments, the coupling strength between the quantum dots has an enhanced impact on the geometric phase during a quasiperiod. This is due to the fact that the expansion of the width of the tunneling channel connecting the two quantum dots accelerates the oscillations of the electron between the quantum dots and makes the length of the evolution path longer. In addition, there is a notable near-zero region in the geometric phase because the stronger coupling between the system and the QPC freezes the electron in one quantum dot and the solid angle enclosed by the evolution path is approximately zero, which is associated with the quantum Zeno effect. For the pure dephasing environment, the geometric phase is suppressed as the dephasing rate increases which is caused only by the phase damping of the system. In the dissipative environment, the geometric phase is reduced with the increase of the relaxation rate which results from both the energy dissipation and phase damping of the system. Our results are helpful for using the geometric phase to construct the fault-tolerant quantum devices based on quantum dot systems in quantum information.
We investigate the effect of environment parameters on the geometric phase of a quantum dot (QD) system interacting with the environment. Specifically, we calculate the effect of two important parameters: the energy difference of the electron in QD and the backaction of the QD to the environment. Our result shows that the geometric phase values are obviously dependent on these parameters. The variance of the geometric phase as functions of the parameters is plotted. We further analyze the physical mechanism of the numerical result.