SEMICLASSICAL AND LARGE QUANTUM NUMBER LIMITS
... implies the limit of large quantum numbers. For negative degrees d, the potentials behave as inverse powers of the coordinate and vanish asymptotically. The spectrum of the Hamiltonian is continuous for positive energies, and bound states with discrete energy eigenvalues occur for E ≤ 0. For d < −2, ...
... implies the limit of large quantum numbers. For negative degrees d, the potentials behave as inverse powers of the coordinate and vanish asymptotically. The spectrum of the Hamiltonian is continuous for positive energies, and bound states with discrete energy eigenvalues occur for E ≤ 0. For d < −2, ...
Unifying Classical and Quantum Key Distillation
... In information-theoretic cryptography, where no assumptions on the adversary’s resources6 are made, distributing keys between distant parties is impossible if only public classical communication channels are available [1, 2]. However, this situation changes dramatically if the parties have access t ...
... In information-theoretic cryptography, where no assumptions on the adversary’s resources6 are made, distributing keys between distant parties is impossible if only public classical communication channels are available [1, 2]. However, this situation changes dramatically if the parties have access t ...
Luttinger Liquids
... bit complicated. The result is however, as expected, that the discontinuity totally disappears, which shows that there are no stable gapless charge excitations in the system. Although there are no gapless fermions in the spectrum, the bosonic excitations are gapless. In this respect the Luttinger mo ...
... bit complicated. The result is however, as expected, that the discontinuity totally disappears, which shows that there are no stable gapless charge excitations in the system. Although there are no gapless fermions in the spectrum, the bosonic excitations are gapless. In this respect the Luttinger mo ...
Gate Tunable Relativistic Mass and Berry’s phase in Topological Insulator
... gated R modulation ratio is , 3–10 in our field effect devices. For Vg 5 0 V, the temperature (T) dependence of the resistance (R(T)) of the Bi2Te3 NR device (Fig. 2b) shows a metallic behavior (R decreases with decreasing T), as previously observed in highly doped samples with bulk-dominated conduc ...
... gated R modulation ratio is , 3–10 in our field effect devices. For Vg 5 0 V, the temperature (T) dependence of the resistance (R(T)) of the Bi2Te3 NR device (Fig. 2b) shows a metallic behavior (R decreases with decreasing T), as previously observed in highly doped samples with bulk-dominated conduc ...
Measurement-based and Universal Blind Quantum Computation
... quantum measurements are inherently not deterministic, one can sometimes ensure the global determinism of the computation using suitable dependencies between measurements. Flow asserts that under a graph-theoretic condition on the entanglement underlying a given computation, it is possible to constr ...
... quantum measurements are inherently not deterministic, one can sometimes ensure the global determinism of the computation using suitable dependencies between measurements. Flow asserts that under a graph-theoretic condition on the entanglement underlying a given computation, it is possible to constr ...
Towards a microscopic Description of classical Solutions in Field
... should be understood as a quantum bound state of proper microscopic degrees of freedom. As a consequence, consistency requires that all the classical features should emerge from these underlying physics. Following this logic, we develop methods to represent classical fields in various examples in te ...
... should be understood as a quantum bound state of proper microscopic degrees of freedom. As a consequence, consistency requires that all the classical features should emerge from these underlying physics. Following this logic, we develop methods to represent classical fields in various examples in te ...
Spectroscopic Selection Rules: The Role of Photon States
... However, many students find the transition moment to be a somewhat obscure quantity that does little to reveal the underlying physics. Furthermore, the journey from the transition moment to a particular selection rule is not always easy. This is especially troublesome when all one wishes to achieve ...
... However, many students find the transition moment to be a somewhat obscure quantity that does little to reveal the underlying physics. Furthermore, the journey from the transition moment to a particular selection rule is not always easy. This is especially troublesome when all one wishes to achieve ...
11th International Conference on Squeezed - icssur 2009
... Wineland’s squeezing parameter as a compatible parameter with time evolution of Q function (S. V. Kashanian) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 88 Atomic parity nonconservation in heavy atoms and observing P and PT violation using NMR shift in a l ...
... Wineland’s squeezing parameter as a compatible parameter with time evolution of Q function (S. V. Kashanian) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 88 Atomic parity nonconservation in heavy atoms and observing P and PT violation using NMR shift in a l ...
Toward a scalable, silicon-based quantum computing architecture
... orthogonal states, only one of those states can be observed, or measured. After measurement, the system is no longer in superposition: the quantum state collapses into the one state measured, and the probability amplitude of all other states goes to is measured, zero. For example, when the state the ...
... orthogonal states, only one of those states can be observed, or measured. After measurement, the system is no longer in superposition: the quantum state collapses into the one state measured, and the probability amplitude of all other states goes to is measured, zero. For example, when the state the ...
PDF
... We consider perception as a term describing a broad range of cognitive functions, one of the simplest of which is sensation. That is, the set of sensory functions will be taken as a subset of the set of perceptual functions. Traditionally, the values of the stimulus that appears in Figure 2 are writ ...
... We consider perception as a term describing a broad range of cognitive functions, one of the simplest of which is sensation. That is, the set of sensory functions will be taken as a subset of the set of perceptual functions. Traditionally, the values of the stimulus that appears in Figure 2 are writ ...
Time-Space Efficient Simulations of Quantum Computations
... randomized computations by quantum computations. Several of the known models only allow measurements at the end of the computation but not during the computation. As another example, the ...
... randomized computations by quantum computations. Several of the known models only allow measurements at the end of the computation but not during the computation. As another example, the ...
Devil physics The baddest class on campus IB Physics
... U-tube, models of icebergs oscillating vertically in the ocean, and motion of a sphere rolling in a concave mirror Simple harmonic motion is frequently found in the context of mechanics (see Physics topic ...
... U-tube, models of icebergs oscillating vertically in the ocean, and motion of a sphere rolling in a concave mirror Simple harmonic motion is frequently found in the context of mechanics (see Physics topic ...
104,18415 (2007)
... guarantee topological protection. The most famous example of this is the magnetic Kitaev lattice, described in the pioneering papers (2, 3) on topological quantum computation. The Kitaev model is an exactly soluble lattice model that carries excitations with both Abelian and non-Abelian anyonic brai ...
... guarantee topological protection. The most famous example of this is the magnetic Kitaev lattice, described in the pioneering papers (2, 3) on topological quantum computation. The Kitaev model is an exactly soluble lattice model that carries excitations with both Abelian and non-Abelian anyonic brai ...
Driven Bose-Hubbard model with a parametrically modulated
... delicate interplay of both the local interaction of the atoms in the lattice and the driving of the global trap allows us to control the dynamical stability of the trapped quantum many-body state. The impact of the atomic interaction on the dynamical stability of the driven quantum many-body state i ...
... delicate interplay of both the local interaction of the atoms in the lattice and the driving of the global trap allows us to control the dynamical stability of the trapped quantum many-body state. The impact of the atomic interaction on the dynamical stability of the driven quantum many-body state i ...
