A single electron spin in a double quantum dot in a magnetic field is considered in terms of a four-level system. By describing the electron motion between the potential minima via spin-conserving tunneling and spin flip caused by a spin-orbit coupling, we inversely engineer faster-than-adiabatic state manipulation operations based on the geometry of four-dimensional rotations. In particular, we show how to transport a qubit among the quantum dots performing simultaneously required spin rotations.
IntroductionDevice architecture based on electrons confined in coupled quantum dots [1-4] is considered as a potential and significant candidate for quantum computing and quantum information processing. The advantages of this architecture rely on the facts that electron spin is a natural qubit with spin-up and spin-down states, mature semiconductor technology may be used, and long coherence times on the scale of microseconds have been achieved in these systems [5,6]. Laboratories use electric, microwave or magnetic fields to manipulate spin states, performing 10 3 -10 5 operations in the spin dephasing time [5-10].Scalability of quantum information devices is a major challenge for any architecture, and it is associated with the capability to transport qubits. In this paper we theoretically explore a four-level model for a spin in a double quantum dot (DQD) aiming at the possibilities to implement fast qubit transport with simultaneous qubit rotations. We achieve this goal for arbitrary rotations by controlling the synchronized time dependences of interdot tunneling and spin-orbit coupling (SOC). We inverse-engineer these time dependences based on our recent work [11] on the control of four-level systems. The method separates population control from control of the phases of the bare state basis [12]. Populations can be mapped onto a four-dimensional (4D) sphere such that their evolution amounts to 4D transformation controlled by the (4D-)rotation Hamiltonian that may be engineered from the target state (in our case via isoclinic rotations and quaternions). A full Hamiltonian can then be constructed from the rotation Hamiltonian to realize the desired phase changes. Arbitrary state manipulations require full flexibility in the Hamiltonian, i.e. the possibility to implement the different Hamiltonian matrix elements with specific time-dependences. In the systems of interest, however, there are constraints that hinder certain manipulations and transitions. In particular, in this paper we examine the Hamiltonian structure that corresponds to combined tunneling and SOC controllable couplings, and deduce the possible transformations.Spin-orbit coupling in semiconductors consists of two main contributions due to the Dresselhaus-and the Bychkov-Rashba-effect. The former is due to the bulk inversion asymmetry of the material and the latter results from the structure inversion asymmetry, produced, e.g. by the confining potential or an external electric field [13]. The practical advantage of the Rashba coupling is the ability to man...