QKD in Standard Optical Telecommunications Networks

To perform Quantum Key Distribution, the mastering of the extremely weak signals carried by the quantum channel is required. Transporting these signals without disturbance is customarily done by isolating the quantum channel from any noise sources using a dedicated physical channel. However, to really profit from this technology, a full integration with conventional network technologies would be highly desirable. Trying to use single photon signals with others that carry an average power many orders of magnitude bigger while sharing as much infrastructure with a conventional network as possible brings obvious problems. The purpose of the present paper is to report our efforts in researching the limits of the integration of QKD in modern optical networks scenarios. We have built a full metropolitan area network testbed comprising a backbone and an access network. The emphasis is put in using as much as possible the same industrial grade technology that is actually used in already installed networks, in order to understand the throughput, limits and cost of deploying QKD in a real network

B_c meson rare decays in the light-cone quark model

We investigate the rare decays $B_c \rightarrow D_s(1968) \ell \bar{\ell}$ and $B_c\rightarrow D_s^*(2317) \ell \bar{\ell}$ in the framework of the light-cone quark model (LCQM). The transition form factors are calculated in the space-like region and then analytically continued to the time-like region via exponential parametrization. The branching ratios and longitudinal lepton polarization asymmetries (LPAs) for the two decays are given and compared with each other. The results are helpful to investigating the structure of $B_c$ meson and to testing the unitarity of CKM quark mixing matrix. All these results can be tested in the future experiments at the LHC.Comment: 9 pages, 11 figures, version accepted for publication in EPJ

Experimental investigation on the influencing factors of a transcritical CO2 heat pump

The concept of “the optimal heat rejection pressure” has attracted wide attention in refrigeration community. Unlike the conventional refrigerants, the heat rejection pressure and temperature of the gas-cooler in the transcritical CO2 cycle are usually decoupled in the transcritical cycle. Besides, there exists an optimal heat rejection pressure under which the maximum cycle efficiency can be achieved. Therefore, the interaction effect between heat rejection pressure and system performance has been studied by many researchers. The heat rejection pressure of the gas-cooler has great impact on the COP of the transcritical CO2 system, but the investigation on the influence factors of the heat rejection pressure is quite rare in open literature. In this paper, the effects of the water inlet temperatures and the water flow rates on the heat rejection pressure of a water-to-water transcritical CO2 refrigeration heat pump with single-stage expansion system have been investigated. Furthermore, the operation parameters and the performance of the system are also evaluated

Design and Setup of the Micro-Turboexpander Transcritical CO2 System

As the potential Eco-friendly refrigerant, CO2 regains more and more attentions. It has various advantages over conventional refrigerants, such as non-flammability, non-toxicity, high volumetric refrigerant capacity and excellent heat transfer properties. Because the heat rejection temperature in a transcritical CO2 heat pump or a transcritical CO2 refrigeration system is higher than the critical temperature of CO2, the transcritical vapor compression cycle becomes the best choice for transcritical CO2 systems. However, the relative low COP caused by the throttle valve limited the further development. The replacement of a throttle valve with a turboexpander, an ejector or a vortex tube is leading to the way for improving the COP of a transcritical CO2 system. With the advantages of high efficiency, high compactness, high reliability and long-life time, turboexpanders have been widely used in gas lique faction devices (below 120K) and most of the reverse Brayton refrigeration systems. It is also one of the most ideal expansion devices for transcritical CO2 systems. However, its applications are limited by the difficulties of high pressure and super high rotating speed operation. With the development of manufacturing technology and gas bearing technology, it becomes possible to use turboexpanders in transcriticalCO2 systems. In this paper, two turboexpanders with 10 mm radial reaction turbine wheel and 9 mm rotor diameter were designed for the 15 kW transcritical CO2 refrigeration system, and the rotating speed is about 200 krpm.The proposed turboexpanders outlet states are CO2 two-phase flow and subcooled CO2 liquid flow, respectively. This study will lay a foundation for the application of turboexpanders in transcritical CO2 systems

Darboux Transformations for a Lax Integrable System in 2n2n-Dimensions

A $2n$-dimensional Lax integrable system is proposed by a set of specific spectral problems. It contains Takasaki equations, the self-dual Yang-Mills equations and its integrable hierarchy as examples. An explicit formulation of Darboux transformations is established for this Lax integrable system. The Vandermonde and generalized Cauchy determinant formulas lead to a description for deriving explicit solutions and thus some rational and analytic solutions are obtained.Comment: Latex, 14 pages, to be published in Lett. Math. Phy

Leptogenesis in the type III seesaw mechanism

It is shown that the type III seesaw mechanism proposed recently can have certain advantages over the conventional (or type I) seesaw mechanism for leptogenesis. In particular a resonant enhancement of leptogenesis via heavy quasi-Dirac right-handed neutrino pairs can occur without a special flavor form or "texture" of the mass matrices being assumed. Some of the requirements for neutrino mixing and leptogenesis are effectively decoupled.Comment: 12 pages including one figure, several references adde

D-concurrence bounds for pair coherent states

The pair coherent state is a state of a two-mode radiation field which is known as a state with non-Gaussian wave function. In this paper, the upper and lower bounds for D-concurrence (a new entanglement measure) have been studied over this state and calculated.Comment: 11 page

J/ψ+c+cˉJ/\psi + c + \bar{c} Photoproduction in e+e−e^+ e^- Scattering

We investigate the $J/\psi$ + c + $\bar{c}$ photoproduction in $e^+ e^-$ collision at the LEP II energy. The physical motivations for this study are: 1) such next-to-leading order(NLO) process was not considered in previous investigations of $J/\psi$ photoproduction in $e^+ e^-$ interaction, and it is worthwhile to do so in order to make sound predictions for experimental comparison; 2) from recent Belle experiment results, the process with same final states at the $B$ factory has a theoretically yet unexplainable large fraction; hence it is interesting to see what may happen at other colliders; 3) the existing LEP data are marginal in observing such process, and at the planed Linear Colliders(LCs) this process can be measured with high accuracy; 4) it is necessary to take this process into consideration in the aim of elucidating the quarkonium production mechanism, especially in testing the universality of NRQCD nonperturbative matrix elements via $J/\psi$ photoproduction in electron-position collisions.Comment: 15 pages, 3 figure

Fermi-surface reconstruction involving two Van Hove singularities across the antiferromagnetic transition in BaFe2As2

We report an angle-resolved photoemission study of BaFe2As2, a parent compound of iron-based superconductors. Low-energy tunable excitation photons have allowed the first observation of a saddle-point singularity at the Z point, as well as the Gamma point. With antiferromagnetic ordering, both of these two van Hove singularities come down below the Fermi energy, leading to a topological change in the innermost Fermi surface around the kz axis from cylindrical to tear-shaped, as expected from first-principles calculation. These singularities may provide an additional instability for the Fermi surface of the superconductors derived from BaFe2As2.Comment: 14 pages, 4 figures, 1 tabl