Type II InAs/GaAsSb quantum dots: Highly tunable exciton geometry
... excited state transition at 1.168 eV (FWHM 29 meV). The intensity of the main peak ranges from 79% of the total emission at 0 V to 94% at 3 V. Therefore, from now on we focus only on the fundamental transition. Figure 2(b) shows how from 40 to 110 kV cm1 the experimental peak energy shifts by 13 ...
... excited state transition at 1.168 eV (FWHM 29 meV). The intensity of the main peak ranges from 79% of the total emission at 0 V to 94% at 3 V. Therefore, from now on we focus only on the fundamental transition. Figure 2(b) shows how from 40 to 110 kV cm1 the experimental peak energy shifts by 13 ...
Anyons and the quantum Hall effect— A pedagogical
... satisfy Schroedinger’s wave equation. And second, these wave functions should satisfy certain symmetry properties with respect to the exchange of identical particles. For fermions the wave function should be anti-symmetric, for bosons it should be symmetric. It is impossible to overrate the importan ...
... satisfy Schroedinger’s wave equation. And second, these wave functions should satisfy certain symmetry properties with respect to the exchange of identical particles. For fermions the wave function should be anti-symmetric, for bosons it should be symmetric. It is impossible to overrate the importan ...
A continued fraction resummation form of bath
... is calculated using the RQKE rates, which is also compared with the exact stochastic path integral result.39,40 In Sec. VI, we summarize our studies. ...
... is calculated using the RQKE rates, which is also compared with the exact stochastic path integral result.39,40 In Sec. VI, we summarize our studies. ...
entanglement properties of quantum many
... Bipartite (two-party) entanglement of pure and mixed states has received thorough study, especially for the case that the two subsystems are two-level systems or Pauli spins. (This is of course the case of most immediate concern for quantum computation, where the two-level computing elements are cal ...
... Bipartite (two-party) entanglement of pure and mixed states has received thorough study, especially for the case that the two subsystems are two-level systems or Pauli spins. (This is of course the case of most immediate concern for quantum computation, where the two-level computing elements are cal ...
IOSR Journal of Applied Physics (IOSR-JAP) e-ISSN: 2278-4861.
... temperature with random values 1 or -1(this is called the hot start). The Monte Carlo method consists to choose randomly a spin to flip. The chosen spin is flipped, if is favourable for the energy. When the energy becomes stable, the system reached the thermalisation, then configurations are determi ...
... temperature with random values 1 or -1(this is called the hot start). The Monte Carlo method consists to choose randomly a spin to flip. The chosen spin is flipped, if is favourable for the energy. When the energy becomes stable, the system reached the thermalisation, then configurations are determi ...
Spin-Orbit Interactions in Topological Insulators
... Hall insulator is gaped in the bulk. However, in contrast to the quantum Hall insulator there exists two sets of edge states. One for each spin direction, and these propagates in opposite directions. direction it has to reverse it’s spin, which would require scattering against magnetic impurities. T ...
... Hall insulator is gaped in the bulk. However, in contrast to the quantum Hall insulator there exists two sets of edge states. One for each spin direction, and these propagates in opposite directions. direction it has to reverse it’s spin, which would require scattering against magnetic impurities. T ...
Time reversal and the symplectic symmetry of the electron spin.
... more stringent than the requirement that the Hamiltonian display SP (N) symmetry. However, if the Hamiltonian H[S, P] includes any “dipole moment” operators P, the non-trivial commutators between the magnetic moments and electric dipoles destroy the closure and time reversal ceases to exist as a wel ...
... more stringent than the requirement that the Hamiltonian display SP (N) symmetry. However, if the Hamiltonian H[S, P] includes any “dipole moment” operators P, the non-trivial commutators between the magnetic moments and electric dipoles destroy the closure and time reversal ceases to exist as a wel ...
Adiabatic State Preparation of Interacting Two-Level Systems R. T. Brierley, C. Creatore,
... ensemble of many two level systems. The interaction lifts the degeneracy of the eigenstates of the Hamiltonian, Eq. (1), and causes the level crossings at which state transfer occurs to separate in time. As in the bosonic Josephson junction [36,40–42], the isolation of each degeneracy increases the ...
... ensemble of many two level systems. The interaction lifts the degeneracy of the eigenstates of the Hamiltonian, Eq. (1), and causes the level crossings at which state transfer occurs to separate in time. As in the bosonic Josephson junction [36,40–42], the isolation of each degeneracy increases the ...
Testing quantum-like models of judgment for conjunction
... The vector space is equipped with a scalar product, thus becoming a Hilbert space: for two vectors W and X, the scalar product W · X is a complex number. The order of the vectors within a scalar product here matters: X · W is the complex conjugate of W · X. The above bases are supposed to be orthogo ...
... The vector space is equipped with a scalar product, thus becoming a Hilbert space: for two vectors W and X, the scalar product W · X is a complex number. The order of the vectors within a scalar product here matters: X · W is the complex conjugate of W · X. The above bases are supposed to be orthogo ...
Answers/solutions
... Table 11.2a + Hund’s rule 6S which has state 6S5/2 . (Half-filled). Z=24, ground configuration: 1s22s22p63s23p63d6 Table 11.2a + Hund’s rule5D. +more than half-filled ground state symbol: 5D4 Z=25, ground configuration: 1s22s22p63s23p63d7 Table 11.2a + Hund’s rule4F. +more than half-filled ...
... Table 11.2a + Hund’s rule 6S which has state 6S5/2 . (Half-filled). Z=24, ground configuration: 1s22s22p63s23p63d6 Table 11.2a + Hund’s rule5D. +more than half-filled ground state symbol: 5D4 Z=25, ground configuration: 1s22s22p63s23p63d7 Table 11.2a + Hund’s rule4F. +more than half-filled ...
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... Heisenberg indeterminacy principle (we cannot measure simultaneously the momentum and the position of an electron). The phenomenon by which electrons change into photons by rotating 180 degrees in an extra dimension (Icke, ...
... Heisenberg indeterminacy principle (we cannot measure simultaneously the momentum and the position of an electron). The phenomenon by which electrons change into photons by rotating 180 degrees in an extra dimension (Icke, ...
Quantum Annealing with Markov Chain Monte Carlo Simulations
... ψ|Qa |ψ, a = 1, 2, . . . , r. Statistically, we may perform measurements on M for the quantum system multiple times to obtain measurement data and infer the quantum state from the data. For a quantum system at a given time point, its state vector comprises all information about the system in the s ...
... ψ|Qa |ψ, a = 1, 2, . . . , r. Statistically, we may perform measurements on M for the quantum system multiple times to obtain measurement data and infer the quantum state from the data. For a quantum system at a given time point, its state vector comprises all information about the system in the s ...
Multiphoton antiresonance M. I. Dykman and M. V. Fistul
... periods 2 / 共g兲 are the same.10 When the motion is quantized, 共g兲 gives the distance between the energy levels. Therefore if, for some ␦ and , two levels that correspond to the external and internal trajectories coincide with each other, many levels will coincide pairwise as well. Level splitti ...
... periods 2 / 共g兲 are the same.10 When the motion is quantized, 共g兲 gives the distance between the energy levels. Therefore if, for some ␦ and , two levels that correspond to the external and internal trajectories coincide with each other, many levels will coincide pairwise as well. Level splitti ...
