On the role of the electron-electron interaction in two-dimensional
... good convergence only feasible for even fewer particles [36]. The different varieties of the quantum Monte Carlo methods are very powerful and yield virtually exact results. However, only the state with the lowest energy for each given symmetry is easily obtained and there is no straightforward way ...
... good convergence only feasible for even fewer particles [36]. The different varieties of the quantum Monte Carlo methods are very powerful and yield virtually exact results. However, only the state with the lowest energy for each given symmetry is easily obtained and there is no straightforward way ...
QUANTUM ALGORITHMS FOR ELEMENT DISTINCTNESS∗ 1
... per bound shows that element distinctness is significantly easier than sorting for a quantum computer, in contrast to the classical case. In Section 4, we consider the case where f is ordered (monotone non-decreasing): f (1) ≤ f (2) ≤ · · · ≤ f (N ). In this case, the quantum complexity of claw-fin ...
... per bound shows that element distinctness is significantly easier than sorting for a quantum computer, in contrast to the classical case. In Section 4, we consider the case where f is ordered (monotone non-decreasing): f (1) ≤ f (2) ≤ · · · ≤ f (N ). In this case, the quantum complexity of claw-fin ...
quantum computer graphics algorithms
... there is no additional information about the search condition, the best classical algorithm is a brute-force search, meaning that the elements are sequentially tested against the search condition. For a list of N elements, this algorithm executes an average of N / 2 comparisons. By exploiting the ad ...
... there is no additional information about the search condition, the best classical algorithm is a brute-force search, meaning that the elements are sequentially tested against the search condition. For a list of N elements, this algorithm executes an average of N / 2 comparisons. By exploiting the ad ...
PHOTONIC ENTANGLEMENT: NEW SOURCES AND NEW APPLICATIONS JI ˇ R´
... Einstein, Podolsky and Rosen published in 1935 a paper [2] that described a Gedanken experiment concerning correlations between quantum particles. They considered a couple of particles that have been allowed to interact in the past, and as a consequence, show certain correlations in position and mom ...
... Einstein, Podolsky and Rosen published in 1935 a paper [2] that described a Gedanken experiment concerning correlations between quantum particles. They considered a couple of particles that have been allowed to interact in the past, and as a consequence, show certain correlations in position and mom ...
11th International Conference on Squeezed - icssur 2009
... Quantum treatment of the time-dependent coupled oscillators under the action of a random force (M. S. Abdalla) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 Quantum correlations and device-independent quantum information protocols (A. Acı́n) . . . . . . . . . ...
... Quantum treatment of the time-dependent coupled oscillators under the action of a random force (M. S. Abdalla) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 Quantum correlations and device-independent quantum information protocols (A. Acı́n) . . . . . . . . . ...
Evolving Quantum circuits - Portland State University
... [6,7,18,42,45]. This result is different from binary reversible logic, where the minimum universal gate is 3*3 [19,44] (all quantum gates are reversible and reversible gates have the same number of inputs and outputs and are one-to-one mappings, k*k gate has k inputs and k outputs). An interesting q ...
... [6,7,18,42,45]. This result is different from binary reversible logic, where the minimum universal gate is 3*3 [19,44] (all quantum gates are reversible and reversible gates have the same number of inputs and outputs and are one-to-one mappings, k*k gate has k inputs and k outputs). An interesting q ...
On the Study of Quantum Properties of Space-Time with
... on proton decay by keeping under observation a large number of protons (so that the experiments measure the probability that one among many protons decay). As the analogy with proton decay in granduni cation suggests, Planck-length phenomenology is not impossible, but it is extremely hard. While opp ...
... on proton decay by keeping under observation a large number of protons (so that the experiments measure the probability that one among many protons decay). As the analogy with proton decay in granduni cation suggests, Planck-length phenomenology is not impossible, but it is extremely hard. While opp ...
Selection rules for nonradiative carrier relaxation processes in
... pairs, a biexciton, in an excited state [Fig. 1(b)]. The relaxation of the excited biexciton can then be studied experimentally by detecting emission due to a second e-h pair recombination, which occurs after the excited biexciton relaxes nonradiatively to various lower-energy biexciton configuratio ...
... pairs, a biexciton, in an excited state [Fig. 1(b)]. The relaxation of the excited biexciton can then be studied experimentally by detecting emission due to a second e-h pair recombination, which occurs after the excited biexciton relaxes nonradiatively to various lower-energy biexciton configuratio ...
1. Introduction - Université de Rennes 1
... Future developments of this work will involve several directions. A first extension will concern the investigation of other spatial configurations: other boundary conditions, whole-space case, or space dimension greater than one. We will also investigate the entropy minimization problem with constra ...
... Future developments of this work will involve several directions. A first extension will concern the investigation of other spatial configurations: other boundary conditions, whole-space case, or space dimension greater than one. We will also investigate the entropy minimization problem with constra ...
Instructions for use Title Coulomb staircase and total spin
... negative bias and reflects the degeneracy of the states relevant to the transition. This has been shown theoretically first for the case with a single orbit18,19 and extended13 to the case with M orbits (M ⬎1). The saturation current at the transition between N and N⫹1 for the positive and negative ...
... negative bias and reflects the degeneracy of the states relevant to the transition. This has been shown theoretically first for the case with a single orbit18,19 and extended13 to the case with M orbits (M ⬎1). The saturation current at the transition between N and N⫹1 for the positive and negative ...
