Pilot's manual/flight working directions for the P-39Q-1 Airacobra

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55 V and Vsd = 8 μV (−300 μV) is shown in Fig. 11a (b). In this region, where (NL , NR ) transits from (5, 3) to (6, 4), the line of the excited state clearly shows the antibonding states. The estimated tunnel coupling energy is 120 μeV. This tunnel coupling energy can be controlled by controlling Vc and the magnetic field. 30 Yasuhiro Tokura et al. Fig. 12. Schematic of coupled 1D dots with ferromagnetic electrodes magnetized in antiparallel configuration. 3 Double QD with Slanting Zeeman Field Here, we present a realization of a two-qubit gate based on the two coupled dots discussed in Sect.

Gossard, Phys. Rev. Lett. 91, 016802 (2003) 16 9. R. Hanson, B. K. H. M. P. Kouwenhoven, Phys. Rev. Lett. 91, 196802 (2003) 16, 18, 22 10. H. Willems van Beveren, R. T. L. P. K. Vandersypen, New J. Phys. 7, 182 (2005) 16 11. A. Kogan, S. Amasha, D. Goldhaber-Gordon, G. A. Kastner, H. Shtrikman, Phys. Rev. Lett. 93, 166602 (2004) 16 12. T. G. van der Wiel, T. Maruyama, S. Tarucha, in Proc. Int. Symp. on Mesoscopic Superconductivity and Spintronics 2004 (MS+S2004) (World Scientific, Singapore, 2005) 16, 18 13.

Thus, the effective ESR the lowest-order perturbation, Co,1,σ = e1 − o1 +ε0z σ Hamiltonian (1) is obtained. It should be noted that addressing an individual qubit is easy since the ESR field is very local and can be reproduced for each dot. In the analysis, we used the material parameters of GaAs and a confinement energy of the order of 1 meV, which corresponds to e1|z|o1 ∼ 24 nm [26]. 5 V/cm, and bSL ∼ 1 T/μm. The electric field required to achieve a 1-mT oscillating field using micromagnets is about ten times smaller than that using the SO interaction [24].

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