Highly doubly excited S states of the helium atom
... with real b, B. A typical choice for b is b = l / N or smaller ( N is the principal quantum number of the HeC ion to which the Rydberg series converges). By solving (8) we get a large number of converged complex eigenvalues that represent the doubly excited resonances. 2.2. Numerical computation of ...
... with real b, B. A typical choice for b is b = l / N or smaller ( N is the principal quantum number of the HeC ion to which the Rydberg series converges). By solving (8) we get a large number of converged complex eigenvalues that represent the doubly excited resonances. 2.2. Numerical computation of ...
Experiments with Entangled Photons Bell Inequalities, Non-local Games and Bound Entanglement
... the concepts on which classical physics is based. For instance, it permits persistent correlations between classically separated systems, that are termed as entanglement. To circumvent these problems and explain entanglement, hidden variables theories–based on undiscovered parameters–have been devis ...
... the concepts on which classical physics is based. For instance, it permits persistent correlations between classically separated systems, that are termed as entanglement. To circumvent these problems and explain entanglement, hidden variables theories–based on undiscovered parameters–have been devis ...
Causal structural realism in canonical quantum gravity
... rather than ‘only’ a quantized version of GR.) Indeed, the dynamics of the theory can be fully understood in terms of transition probability amplitudes for spin network states. The transition amplitudes do not depend explicitly on time and cannot be understood as transition amplitudes between states ...
... rather than ‘only’ a quantized version of GR.) Indeed, the dynamics of the theory can be fully understood in terms of transition probability amplitudes for spin network states. The transition amplitudes do not depend explicitly on time and cannot be understood as transition amplitudes between states ...
Maritime Applications of Quantum Computation
... Each lattice Qk ∈ Z will be used to store a copy of the image so that, by the end of the recording procedure, Z will be a set of n3 lattices all of which have been prepared identically. We must prepare several identical copies of the same image because, as exposed in subsection II-3, retrieving info ...
... Each lattice Qk ∈ Z will be used to store a copy of the image so that, by the end of the recording procedure, Z will be a set of n3 lattices all of which have been prepared identically. We must prepare several identical copies of the same image because, as exposed in subsection II-3, retrieving info ...
Axiomatic description of mixed states from Selinger`s CPM
... considering their preparation procedures as a special case of quantum channels. Since for each †-compact category Selinger’s construction provides another †-compact category, it doesn’t truly provide a profound structural grasp on quantum mixedness in the usual axiomatic sense. In this paper we obse ...
... considering their preparation procedures as a special case of quantum channels. Since for each †-compact category Selinger’s construction provides another †-compact category, it doesn’t truly provide a profound structural grasp on quantum mixedness in the usual axiomatic sense. In this paper we obse ...
Exponential algorithmic speedup by quantum walk Andrew M. Childs, Richard Cleve, Enrico Deotto,
... At each vertex, we query the oracle and move to one of the two unvisited adjacent vertices. After n steps, we reach the central column and then proceed moving to unvisited adjacent vertices in the right tree, checking the degree at each step. If we discover that after k steps we are again at a centr ...
... At each vertex, we query the oracle and move to one of the two unvisited adjacent vertices. After n steps, we reach the central column and then proceed moving to unvisited adjacent vertices in the right tree, checking the degree at each step. If we discover that after k steps we are again at a centr ...
Quantum mechanical modeling of the CNOT (XOR) gate
... So, for eq. (27), the global-rotations-symmetry-requirement implies (as it can be easily seen): [Ŝ1n , σ̂1z ] = 0, (34a) [Ŝ2n , σ̂2x ] = 0. ...
... So, for eq. (27), the global-rotations-symmetry-requirement implies (as it can be easily seen): [Ŝ1n , σ̂1z ] = 0, (34a) [Ŝ2n , σ̂2x ] = 0. ...
