The hyperfine structure of the 1 3 g state of Na2
... state from intermediate A 1 兺 ⫹ u ⬃b 兿 1u mixed levels. They successfully explained the hyperfine splittings with the Fermi contact interaction b F I•S1 term. We report here the hyperfine structure of transitions to low-N levels of the Na2 1 3 ⌬ g state. This structure turns out to be much more comp ...
... state from intermediate A 1 兺 ⫹ u ⬃b 兿 1u mixed levels. They successfully explained the hyperfine splittings with the Fermi contact interaction b F I•S1 term. We report here the hyperfine structure of transitions to low-N levels of the Na2 1 3 ⌬ g state. This structure turns out to be much more comp ...
Quantum Computational Complexity - Cheriton School of Computer
... theories should be considered in the context of computational complexity. In particular, quantum mechanics is a clear candidate for a physical theory to have the potential for implications, if not to computational complexity then at least to computation more generally. Given the steady decrease in t ...
... theories should be considered in the context of computational complexity. In particular, quantum mechanics is a clear candidate for a physical theory to have the potential for implications, if not to computational complexity then at least to computation more generally. Given the steady decrease in t ...
Born approximation - BYU Physics and Astronomy
... A. To develop a formalism where we express the wave function in terms of Green’s functions B. To use Helmholtz equation instead of Schrödinger equation C. To find an approximate expression for when far away from the scattering center for a given potential V D. To express the scattering factor in t ...
... A. To develop a formalism where we express the wave function in terms of Green’s functions B. To use Helmholtz equation instead of Schrödinger equation C. To find an approximate expression for when far away from the scattering center for a given potential V D. To express the scattering factor in t ...
around the notion of state and the superposition principle en torno a
... identity. In this context, the description of mechanical systems from the can be made perspective of states [9]. A body in a gravitational can be described field fall in free from its state of motion; is defined it as the different ways of being the body in the gravitational field at each instant of ...
... identity. In this context, the description of mechanical systems from the can be made perspective of states [9]. A body in a gravitational can be described field fall in free from its state of motion; is defined it as the different ways of being the body in the gravitational field at each instant of ...
Transport Properties of Interacting Edge Modes in 2D Topological
... the second corresponds to the existence of topologically protected edge states, vulgo a quantum spin Hall insulator. From another persepective, we see, that the topologically trivial and non-trivial cases are distinguished by whether the chemical potential crosses the bands an even or and odd number ...
... the second corresponds to the existence of topologically protected edge states, vulgo a quantum spin Hall insulator. From another persepective, we see, that the topologically trivial and non-trivial cases are distinguished by whether the chemical potential crosses the bands an even or and odd number ...
Entanglement Entropy at Infinite-Randomness Fixed Points in Higher Dimensions Yu-Cheng Lin,
... Extensive studies have been devoted recently to understanding ground state entanglement in quantum manybody systems [1]. In particular, the behavior of various entanglement measures at or near quantum phase transitions has been of special interest. One of the widely used entanglement measures is the ...
... Extensive studies have been devoted recently to understanding ground state entanglement in quantum manybody systems [1]. In particular, the behavior of various entanglement measures at or near quantum phase transitions has been of special interest. One of the widely used entanglement measures is the ...
72 063623 (2005) .
... ity decay for the three cases and detailed parameters are indicated in the caption. As we choose parameters as K = 2, gc = 0.2, the classical system is nearly integrable where the phase space is full of periodic and quasiperiodic orbits. We found Gaussian decay for the fidelity of single initial coh ...
... ity decay for the three cases and detailed parameters are indicated in the caption. As we choose parameters as K = 2, gc = 0.2, the classical system is nearly integrable where the phase space is full of periodic and quasiperiodic orbits. We found Gaussian decay for the fidelity of single initial coh ...
An introduction to topological phases of electrons
... Note that (c) obviously implies (a) and (b), since then W = g(u(1), v(1)) − g(u(0), v(0)). To show that (b) implies (a), suppose (b) is true and (a) is not. Then there are two paths γ1 , γ2 that have different integrals but the same endpoints. Form a new path γ so that, as t goes from 0 to 12 , γ1 i ...
... Note that (c) obviously implies (a) and (b), since then W = g(u(1), v(1)) − g(u(0), v(0)). To show that (b) implies (a), suppose (b) is true and (a) is not. Then there are two paths γ1 , γ2 that have different integrals but the same endpoints. Form a new path γ so that, as t goes from 0 to 12 , γ1 i ...
Quantum Correlations in Information Theory
... quantum entanglement, i.e. peculiar correlations described by quantum laws which are shared, for example, between the sender and the receiver of a message. However, it has been recently shown that entanglement is not the most general form of quantum correlations. Even unentangled states of compound ...
... quantum entanglement, i.e. peculiar correlations described by quantum laws which are shared, for example, between the sender and the receiver of a message. However, it has been recently shown that entanglement is not the most general form of quantum correlations. Even unentangled states of compound ...