Mutually unbiased bases, orthogonal Latin squares, and hidden
... only if k = 1, i.e., nm = nm ⬘ for exactly one m. This condition applied to d2 orthogonal operators, defines a complete set of orthogonal squares. To see this, take d2 orthogonal operators B̂n0共b兲,. . .,nd共b兲 with b = 1 , . . . , d2 and consider d + 1 squares defined by their indices nm共b兲 for a fix ...
... only if k = 1, i.e., nm = nm ⬘ for exactly one m. This condition applied to d2 orthogonal operators, defines a complete set of orthogonal squares. To see this, take d2 orthogonal operators B̂n0共b兲,. . .,nd共b兲 with b = 1 , . . . , d2 and consider d + 1 squares defined by their indices nm共b兲 for a fix ...
Exciton Beats in GaAs Quantum Wells: Bosonic Representation and Collective... J. Fern´andez-Rossier and C. Tejedor
... used to coherently control the HX density in a GaAs QW [7,10]. We also analyze the case where a single pulse excites both the LX and HX states and argue that the resulting beats [1–4,11,12] are not due to (single-exciton) quantum interference, as advocated by few-level models, but to polarization in ...
... used to coherently control the HX density in a GaAs QW [7,10]. We also analyze the case where a single pulse excites both the LX and HX states and argue that the resulting beats [1–4,11,12] are not due to (single-exciton) quantum interference, as advocated by few-level models, but to polarization in ...
Integrated optomechanics and linear optics quantum circuits
... – Inversely proportional to the gap make small ...
... – Inversely proportional to the gap make small ...
You obtained your required density profile data
... Therefore we can calculate just the average pressure using DFT. 3)Also figures 2-7 have been plotted using the derived equation although in which the results of the local densities results of the perturbative fundamental measure density functional theory have been used. Finally, I have calculated th ...
... Therefore we can calculate just the average pressure using DFT. 3)Also figures 2-7 have been plotted using the derived equation although in which the results of the local densities results of the perturbative fundamental measure density functional theory have been used. Finally, I have calculated th ...
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... deforms to the affine space G/T , whose Gromov-Witten invariants vanish (recall that Gromov-Witten invariants are invariant under deformations of the complex structure). However, there is no C∗ -equivariant deformation to an affine space, and in fact the C∗ -equivariant quantum cohomology is non-tri ...
... deforms to the affine space G/T , whose Gromov-Witten invariants vanish (recall that Gromov-Witten invariants are invariant under deformations of the complex structure). However, there is no C∗ -equivariant deformation to an affine space, and in fact the C∗ -equivariant quantum cohomology is non-tri ...
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... Subscribers of the next generation wireless systems will communicate simultaneously, sharing the same frequency band. All around the world 3G mobile systems apply Direct Sequence - Code Division Multiple Access (DS-CDMA) promising due to its high capacity and inherent resistance to interference, hen ...
... Subscribers of the next generation wireless systems will communicate simultaneously, sharing the same frequency band. All around the world 3G mobile systems apply Direct Sequence - Code Division Multiple Access (DS-CDMA) promising due to its high capacity and inherent resistance to interference, hen ...
Holonomic Quantum Computation with Josephson Networks
... 1. Introduction The most common paradigm how to perform a quantum computation is to prepare the quantum register in some initial state and then to apply a well-defined sequence of one-qubit and two-qubit (or, in general, N-qubit) operations. These unitary operations – the so-called quantum gates – t ...
... 1. Introduction The most common paradigm how to perform a quantum computation is to prepare the quantum register in some initial state and then to apply a well-defined sequence of one-qubit and two-qubit (or, in general, N-qubit) operations. These unitary operations – the so-called quantum gates – t ...
Quantum Field Theory on Curved Backgrounds. II
... g, so by the Lemma there is a unique analytic homomorphism ξX : R → G such that d ξX (D) = X. Conversely, if η is an analytic homomorphism of R → G, and if we let X = d η (D), it is obvious that η = ξX . Thus X 7→ ξX is a bijection of g onto the set of analytic homomorphisms R → G. The exponential m ...
... g, so by the Lemma there is a unique analytic homomorphism ξX : R → G such that d ξX (D) = X. Conversely, if η is an analytic homomorphism of R → G, and if we let X = d η (D), it is obvious that η = ξX . Thus X 7→ ξX is a bijection of g onto the set of analytic homomorphisms R → G. The exponential m ...
Quantum-teleportation benchmarks for independent and identically
... The second remark concerns the supremum over the small ball ρθ − ρθ 1 n−1/2+ in definition (3). Why not consider the supremum over all θ as we did in the nonasymptotic case ? The reason is that the global supremum would be overly pessimistic and would be dominated by the region in the parameter ...
... The second remark concerns the supremum over the small ball ρθ − ρθ 1 n−1/2+ in definition (3). Why not consider the supremum over all θ as we did in the nonasymptotic case ? The reason is that the global supremum would be overly pessimistic and would be dominated by the region in the parameter ...