![]() Xiao, W., Xiao, J.L.: Coulomb bound potential quantum rod qubit. Xiao, J.L.: Effect of hydrogen-like impurity on a qubit in quantum pseudodot at finite temperature. Xiao, J.L.: Effects of temperature and hydrogen-like impurity on the coherence time of RbCl parabolic quantum dot qubit. Xiao, J.L.: The effect of magnetic field on RbCl quantum pseudodot qubit. Wiersig, J.: Computation of the coherence time of quantum-dot microcavity lasers including photon-carrier and photon-photon correlations. Tiotsop, M., Fotue, A.J., Fotsin, H.B., Fai, L.C.: Tsallis entropy and decoherence of CsI quantum pseudo dot qubit. Pekar, S.I., Deigen, M.F.: The quantum states and the optical transitions of an electron in a polaron and in a color center in a crystal. Nichol, J.M., Orona, L.A., Harvey, S.P., Fallahi, S., Gardner, G.C., Manfra, M.J., Yacoby, A.: High-fidelity entangling gate for double-quantum-dot spin qubits. Liang, Z.H., Xiao, J.L.: Effect of electric field on RbCl quantum pseudodot qubit. Landau, L.D., Lifshitz, E.M.: Quantum Mechanics (Nonrelativistic Theory), p. Kolodka, R.S., Ramsay, A.J., Skiba-Szymanska, J., Fry, P.W., Liu, H.Y., Fox, A.M., Skolnick, M.S.: Inversion recovery of single quantum-dot exciton based qubit. Khordad, R., Ghanbari, A.: Effect of phonons on optical properties of RbCl quantum pseudodot qubits. Huybrechts, W., Devreese, J.: Phonon-correlation effects in the optical-absorption spectra of free polarons. Huthmacher, L., Stockill, R., Clarke, E., Hugues, M., Le Gall, C., Atatüre, M.: Coherence of a dynamically decoupled quantum-dot hole spin. Hackmann, J., Glasenapp, P., Greilich, A., Bayer, M., Anders, F.B.: Influence of the nuclear electric quadrupolar interaction on the coherence time of hole and electron spins confined in semiconductor quantum dots. Hackens, B., Faniel, S., Gustin, C., Wallart, X., Bollaert, S., Cappy, A., Bayot, V.: Dwell-time-limited coherence in open quantum dots. Goodman, J.J., Draine, B.T., Flatau, P.J.: Application of fast-Fourier-transform techniques to the discrete-dipole approximation. North-Holland, Amsterdam (1972)Įshghi, M., Ikhdair, S.M.: Quantum pseudodots under the influence of external vector and scalar fields. 118(17), 17 (2017)ĭevreese, J.T.: Polarons in Ionic Crystals and Polar Semiconductors, p. 118, 92–103 (2018)ĭelteil, A., Sun, Z., Fält, S., Imamoğlu, A.: Realization of a cascaded quantum system: heralded absorption of a single photon qubit by a single-electron charged quantum dot. 50(2), 93–105 (2018)Ĭhen, Y.J., Song, H.T., Xiao, J.L.: Constructiveness and destructiveness of temperature in asymmetric quantum pseudo dot qubit system. N + N − = e − Δ E k T are rare, but not impossible.Azizi, V., Vaseghi, B.: Electromagnetically induced transparency in a quantum pseudo-dot with spin–orbit interaction. įor spin=½ nuclei (such as 1H), the polarization due to spins oriented with the field N − relative to the spins oriented against the field N + is given by the Boltzmann distribution: The return of the longitudinal component of the magnetization to its equilibrium value is termed spin-lattice relaxation while the loss of phase-coherence of the spins is termed spin-spin relaxation, which is manifest as an observed free induction decay (FID). The generated transverse magnetization can then induce a signal in an RF coil that can be detected and amplified by an RF receiver. The RF pulses cause the population of spin-states to be perturbed from their thermal equilibrium value. They become abruptly phase coherent when they are hit by radiofrequency (RF) pulses at the resonant frequency, created orthogonal to the field. At thermal equilibrium, nuclear spins precess randomly about the direction of the applied field. This field makes the magnetic dipole moments of the sample precess at the resonance ( Larmor) frequency of the nuclei. In MRI and NMR spectroscopy, an observable nuclear spin polarization ( magnetization) is created by a homogeneous magnetic field. Decay of nuclear spin polarization in MRI and NMR
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