Excitation of high angular momentum Rydberg states
... the smallest sensitivity to static electric fields, the greatest collisional anisotropy and the longest radiative lifetimes of all states within a given n manifold. Several papers have suggested that these states are ideally suited to the study of various phenomena; for example, the modified spectra ...
... the smallest sensitivity to static electric fields, the greatest collisional anisotropy and the longest radiative lifetimes of all states within a given n manifold. Several papers have suggested that these states are ideally suited to the study of various phenomena; for example, the modified spectra ...
6 Theory of the topological Anderson insulator
... simulations of a HgTe quantum well [81, 59]. The combination of a random potential and quadratic momentum terms in the Dirac Hamiltonian can change the sign of the topological mass, thereby transforming a non-inverted quantum well (without edge states in the band gap) into an inverted quantum well ( ...
... simulations of a HgTe quantum well [81, 59]. The combination of a random potential and quadratic momentum terms in the Dirac Hamiltonian can change the sign of the topological mass, thereby transforming a non-inverted quantum well (without edge states in the band gap) into an inverted quantum well ( ...
Hong-Ou-Mandel interference mediated by the magnetic plasmon waves in a three-dimensional
... 1155nm pointed by the green arrows in both experimental and stimulated result. This mode correspond to the second MPW with the phase difference equal to 2π, which can also be regarded as the second excited spin wave-like mode. Its magnetic field distribution is shown in Fig. 2(c). The observation of ...
... 1155nm pointed by the green arrows in both experimental and stimulated result. This mode correspond to the second MPW with the phase difference equal to 2π, which can also be regarded as the second excited spin wave-like mode. Its magnetic field distribution is shown in Fig. 2(c). The observation of ...
Wigner and Nambu–Goldstone Modes of Symmetries
... — in particular, they form the same type of a multiplet — as the generators Q̂a of the broken symmetries. • Finally, the scattering amplitudes involving low-momentum Goldstone particle vanish as O(p) when the momentum pµ of the Goldstone particle goes to zero. If multiple Goldstone particles are inv ...
... — in particular, they form the same type of a multiplet — as the generators Q̂a of the broken symmetries. • Finally, the scattering amplitudes involving low-momentum Goldstone particle vanish as O(p) when the momentum pµ of the Goldstone particle goes to zero. If multiple Goldstone particles are inv ...
Nonabelions in the fractional quantum hall effect
... try to distinguish "particle-like" from "collective" excitations, the latter having Bose statistics and being typically related to fluctuations of conserved quantities such as charge and spin, thus being neutral and having spin zero or one. The other excitations have either non-trivial charge, spin ...
... try to distinguish "particle-like" from "collective" excitations, the latter having Bose statistics and being typically related to fluctuations of conserved quantities such as charge and spin, thus being neutral and having spin zero or one. The other excitations have either non-trivial charge, spin ...
Quantum Error-Correction Codes on Abelian Groups
... Abstract. We prove a general form of bit flip formula for the quantum Fourier transform on finite abelian groups and use it to encode some general CSS codes on these groups. ...
... Abstract. We prove a general form of bit flip formula for the quantum Fourier transform on finite abelian groups and use it to encode some general CSS codes on these groups. ...
Paper
... which we can perform. We shall show that quantum mechanics can be interpreted as theory of such a type. In our approach quantum mechanics is a probabilistic description of physical reality based on the possibility to measure one special chosen (“fundamental”) physical variable – position and its con ...
... which we can perform. We shall show that quantum mechanics can be interpreted as theory of such a type. In our approach quantum mechanics is a probabilistic description of physical reality based on the possibility to measure one special chosen (“fundamental”) physical variable – position and its con ...
Kondo, Fano and Dicke effects in side quantum dots
... is a result of its weak coupling to the conduction electrons mediated by the intermediate quantum-dot 1 (QD1) that is as well at the Kondo regime. This coupling creates a very sharp Kondo peak at QD2 created by depleting, at the vicinity of the Fermi level, the larger Kondo peak of QD1. ...
... is a result of its weak coupling to the conduction electrons mediated by the intermediate quantum-dot 1 (QD1) that is as well at the Kondo regime. This coupling creates a very sharp Kondo peak at QD2 created by depleting, at the vicinity of the Fermi level, the larger Kondo peak of QD1. ...
