Due to the constant mass term and broken degeneracy, we obtain two independent Hilbert spaces. Therefore, we can choose the space K for the definition of the computational basis of the qubit to implement the quantum gates and to make the dynamic control following a genetic algorithm procedure. The wave function in graphene

can be interpreted as a pseudospinor of the sublattice of atom type A or B. In order to visualize the physics evolution due to the gate operation, we calculate the pseudospin Baf-A1 research buy current as the expectation values for Pauli matrices . The selected states that we choose to form the computational basis for the qubit are the selleckchem energies (E j ): E 1/2 = .2492 eV and E −1/2 = .2551 eV (and the corresponding radial

probability distributions is shown in Figure 2a). The energy gap is E 01 = E −1/2 − E 1/2 = 5.838 meV. To achieve transitions between these two states with coherent light, the wavelength required has to be , which is in the range of far-infrared lasers. Also, in controlling the magnetic field B, it is possible to modify this energy gap. We present as a reference point the plot for the density probability and the pseudospin current for the two-dimensional computational basis |0〉 = |ψ 1/2  (Figure 2b) and |1〉 = |ψ − 1/2  (Figure 2c), where a change of direction on pseudospin current and the creation of a hole (null probability near r = 0) is induced when one goes from qubit 0 to1. Figure 2 Diagram of genetic algorithm. Initial population of chromosomes randomly created; the fitness is determined for each chromosome; Dichloromethane dehalogenase WH-4-023 molecular weight parents are selected according to their fitness

and reproduced by pairs, and the product is mutated until the next generation is completed to perform the same process until stop criterion is satisfied. Quantum control: time-dependent potentials First of all, we have to calculate the matrix representation of the time-dependent interactions in the QD basis. Then, we have to use the interaction picture to obtain the ordinary differential equation (ODE) for the time-dependent coefficient which is the probability of being in a state of the QD at time t and finally obtaining the optimal parameter for gate operation. Electric field: oscillating These transitions can be induced by a laser directed to the QD carrying a wavelength that resonates with the qubit states in order to trigger and control transitions in the qubit subspace. We introduce an electric dipole interaction [7] using a time periodic Hamiltonian with frequency ω: V laser(t) = e ϵ ( t ) r, with parameters ϵ ( t ) = ϵ 0 cos ωt, ϵ 0  = ϵ 0(cos ρ, sin ρ), and r = r(cos φ, sin φ), the term ρ is the direction and ϵ 0 is the magnitude of the electric field and are parameters constant in time. To determine the matrix of dipolar transitions on the basis of the QD states, the following overlap integrals must be calculated: (3) where l and j are the state indices.