41,457 research outputs found

    Coherent Exciton Lasing in ZnSe/ZnCdSe Quantum Wells?

    Full text link
    A new mechanism for exciton lasing in ZnSe/ZnCdSe quantum wells is proposed. Lasing, occurring below the lowest exciton line, may be associated with a BCS-like condensed (coherent) exciton state. This state is most stable at low temperatures for densities in the transition region separating the exciton Bose gas and the coherent exciton state. Calculations show the gain region to lie below the exciton line and to be separated from the absorption regime by a transparency region of width, for example, about 80 meV for a 90 Angstrom ZnSe/Zn_(0.75)Cd_(0.25)Se quantum well. Experimental observation of the transparency region using differential spectroscopy would confirm this picture.Comment: 9 pages + 3 figs contained in 4 postscript files to appear Appl. Phys. Lett. March 13, 199

    Technology, Innovation and Latecomer Strategies: Evidence from the Mobile Handset Manufacturing Sector in China

    Get PDF
    Since the entry of Chinese domestic mobile handset manufacturers in 1998, Chinese domestic suppliers have successfully surpassed the market share of joint ventures (JVs) while direct imports have been largely phased out. By examining China’s mobile handset manufacturing sector as a whole and through case studies, we found several factors that contributed to the success of China’s domestic handset manufacturers which can be classified into three categories: market conditions, competition, and government’s support.

    Field theory in superfluid 3He: What are the lessons for particle physics, gravity and high-temperature superconductivity?

    Full text link
    There are several classes of homogeneous Fermi-systems which are characterized by the topology of the energy spectrum of fermionic quasiparticles: (1) Gapless systems with a Fermi-surface; (2) Systems with a gap in their spectrum; (3) Gapless systems with topologically stable point nodes (Fermi points); and (4) Gapless systems with topologically unstable lines of nodes (Fermi lines). Superfluid 3He-A and electroweak vacuum belong to the universality Class (3). The fermionic quasiparticles (particles) in this class are chiral: they are left-handed or right-handed. The collective bosonic modes of systems of Class (3) are the effective gauge and gravitational fields. The great advantage of superfluid 3He-A is that we can perform experiments using this condensed matter and thereby simulate many phenomena in high energy physics, including axial anomaly, baryoproduction, and magnetogenesis. 3He-A textures induce a nontrivial effective metrics of the space, where the free quasiparticles move along geodesics. With 3He-A one can simulate event horizons, Hawking radiation, rotating vacuum, etc. High-temperature superconductors are believed to belong to Class (4). They have gapless fermionic quasiparticles with a "relativistic" spectrum close to gap nodes, which allows application of ideas developed for superfluid 3He-A.Comment: RevTex file, 8 pages, 5 figures, submitted to Proc. Nat. Ac. Sc. US, modified after referee reports, references are adde

    Diquark in Nona-quark States

    Full text link
    We study the nonaquark states S0(3115)S^0(3115) and S+(3140)S^+(3140) which are reported by KEK-PS (Phys.Lett. B597 (2004) 236; nucl-ex/0310018) by means of the quark model with diquark correlation. The nonaquark states form 1,8,10,10ˉ,27,35ˉ\bf{1},\bf{8},\bf{10},\bar{\bf{10}},\bf{27},\bar{\bf{35}} SU(3) multiplets. The flavor wave functions of all the nonaquark states are constructed through the standard tensor technique. The mass spectrum is studied by using Gell-Mann-Okubo mass formula. Some nonaquark mass sum rules are obtained. We further investigate the decay of S0(3115)S^0(3115) and S+(3140)S^+(3140) under the assumption of "fall-apart" mechanism. It has been found that the main decay mode is ΣNN\Sigma NN rather than ΛNN\Lambda NN which is consistent with experiment. Also we have uniquely determine the flavor wave function of S0(3115)S^0(3115) which belong to 27\bf{27}-plet with the quantum number Y=2,I=1,Iz=1Y=2,I=1,I_z=-1. Whereas the exotic states S+(3140)S^+(3140) can belong to either 27\bf{27}-plet or 35ˉ\bar{\bf{35}}-plet. In the exact SU(3)flavor×SU(3)color×SU(2)spinSU(3)^{flavor}\times SU(3)^{color}\times SU(2)^{spin} limit, both S0(3115)S^0(3115) and S+(3140)S^+(3140) belong to 27{\bf 27}-plet with negative parity. We predict that its flavor structure can be determined by measuring the branch fractions of its decay channels. The experiments to check this prediction are expected.Comment: 23 pages, 8 figures, to appear in Phys. Rev.

    Cusp-scaling behavior in fractal dimension of chaotic scattering

    Full text link
    A topological bifurcation in chaotic scattering is characterized by a sudden change in the topology of the infinite set of unstable periodic orbits embedded in the underlying chaotic invariant set. We uncover a scaling law for the fractal dimension of the chaotic set for such a bifurcation. Our analysis and numerical computations in both two- and three-degrees-of-freedom systems suggest a striking feature associated with these subtle bifurcations: the dimension typically exhibits a sharp, cusplike local minimum at the bifurcation.Comment: 4 pages, 4 figures, Revte

    What kinds of coordinate can keep the Hawking temperature invariant for the static spherically symmetric black hole?

    Full text link
    By studying the Hawking radiation of the most general static spherically symmetric black hole arising from scalar and Dirac particles tunnelling, we find the Hawking temperature is invariant in the general coordinate representation (\ref{arbitrary1}), which satisfies two conditions: a) its radial coordinate transformation is regular at the event horizon; and b) there is a time-like Killing vector.Comment: 10 page

    Heavy Quark Potentials in Some Renormalization Group Revised AdS/QCD Models

    Full text link
    We construct some AdS/QCD models by the systematic procedure of GKN. These models reflect three rather different asymptotics the gauge theory beta functions approach at the infrared region, βλ2,λ3\beta\propto-\lambda^2, -\lambda^3 and βλ\beta\propto-\lambda, where λ\lambda is the 't Hooft coupling constant. We then calculate the heavy quark potentials in these models by holographic methods and find that they can more consistently fit the lattice data relative to the usual models which do not include the renormalization group improving effects. But only use the lattice QCD heavy quark potentials as constrains, we cannot distinguish which kind of infrared asymptotics is the better one.Comment: comparisons with lattice results, qualitative consideration of quantum corrections are added. (accepted by Phys. Rev. D

    Canonical Charmonium Interpretation for Y(4360) and Y(4660)

    Full text link
    In this work, we consider the canonical charmonium assignments for Y(4360) and Y(4660). Y(4660) is good candidate of 53S1\rm 5 ^3S_1 ccˉc\bar{c} state, the possibility of Y(4360) as a 33D1\rm 3 ^3D_1 ccˉc\bar{c} state is studied, and the charmonium hybrid interpretation of Y(4360) can not be excluded completely. We evaluate the e+ee^{+}e^{-} leptonic widths, E1 transitions, M1 transitions and the open flavor strong decays of Y(4360) and Y(4660). Experimental tests for the charmonium assignments are suggested.Comment: 32 pages, 4 figure
    corecore