5,364 research outputs found

    Efficient orthogonal control of tunnel couplings in a quantum dot array

    Full text link
    Electrostatically-defined semiconductor quantum dot arrays offer a promising platform for quantum computation and quantum simulation. However, crosstalk of gate voltages to dot potentials and inter-dot tunnel couplings complicates the tuning of the device parameters. To date, crosstalk to the dot potentials is routinely and efficiently compensated using so-called virtual gates, which are specific linear combinations of physical gate voltages. However, due to exponential dependence of tunnel couplings on gate voltages, crosstalk to the tunnel barriers is currently compensated through a slow iterative process. In this work, we show that the crosstalk on tunnel barriers can be efficiently characterized and compensated for, using the fact that the same exponential dependence applies to all gates. We demonstrate efficient calibration of crosstalk in a quadruple quantum dot array and define a set of virtual barrier gates, with which we show orthogonal control of all inter-dot tunnel couplings. Our method marks a key step forward in the scalability of the tuning process of large-scale quantum dot arrays.Comment: 8 pages, 7 figure

    How Much Does Money Matter in a Direct Democracy?

    Get PDF
    The fine-structure splitting of quantum confined InxGa1-x Nexcitons is investigated using polarization-sensitive photoluminescence spectroscopy. The majority of the studied emission lines exhibits mutually orthogonal fine-structure components split by 100-340 mu eV, as measured from the cleaved edge of the sample. The exciton and the biexciton reveal identical magnitudes but reversed sign of the energy splitting.Original Publication:Supaluck Amloy, Y T Chen, K F Karlsson, K H Chen, H C Hsu, C L Hsiao, L C Chen and Per-Olof Holtz, Polarization-resolved fine-structure splitting of zero-dimensional InxGa1-xN excitons, 2011, PHYSICAL REVIEW B, (83), 20, 201307.http://dx.doi.org/10.1103/PhysRevB.83.201307Copyright: American Physical Societyhttp://www.aps.org

    Equivalent SU(3)fSU(3)_f approaches for two-body anti-triplet charmed baryon decays

    Full text link
    For the two-body anti-triplet charmed baryon decays, there exist two theoretical analyses based on the SU(3)SU(3) flavor (SU(3)fSU(3)_f) symmetry. One is the irreducible SU(3)fSU(3)_f approach (IRA), which depends on the irreducible SU(3)fSU(3)_f representation of the effective Hamiltonian. The other is the topological-diagram approach (TDA), where the decays are drawn to consist of WW-boson emission and WW-boson exchange topologies. We demonstrate that IRA and TDA can be equivalent, such that the IRA parameters can be seen to mix with the TDA topologies. The current observations of Ξc0→Ξ−π+,Ξ−K+,Λ0Kˉ0\Xi_c^0\to \Xi^-\pi^+,\Xi^- K^+,\Lambda^0\bar K^0 might cause theoretical difficulties. With the SU(3)fSU(3)_f symmetry breaking, we explain B(Ξc0→Ξ−π+,Ξ−K+){\cal B}(\Xi_c^0\to\Xi^-\pi^+,\Xi^-K^+). It is found that a specific WW-boson exchange topology denoted by EME_M only appears in Ξc0→BM\Xi_c^0\to{\bf B}M, by which we explain B(Ξc0→Λ0Kˉ0){\cal B}(\Xi_c^0\to\Lambda^0\bar K^0). In addition, we predict B(Ξc0→Σ0Kˉ0,ÎŁ+K−)=(5.8−3.5+4.7,5.4−3.4+4.9)×10−3{\cal B}(\Xi_c^0\to\Sigma^0\bar K^0,\Sigma^+ K^-)= (5.8^{+4.7}_{-3.5},5.4^{+4.9}_{-3.4})\times 10^{-3} for future measurements to test if EME_M can be a significant contribution.Comment: 13 pages, 7 tables, 1 figure, introduction rephrased, reference added, typos correcte

    Pictorial SU(3)fSU(3)_f approach for two-body Ωc\Omega_c weak decays

    Full text link
    We explore two-body non-leptonic weak decays of Ωc0\Omega_c^0 into final states B(∗)M{\bf B}^{(*)}M and B(∗)V{\bf B}^{(*)}V, where B(∗){\bf B}^{(*)} denotes an octet (a decuplet) baryon, and M(V)M(V) represents a pseudoscalar (vector) meson. Based on the SU(3)SU(3) flavor [SU(3)f][SU(3)_f] symmetry, we depict and parameterize the WW-emission and WW-exchange processes using the topological diagram approach, establishing strict SU(3)fSU(3)_f relations for possible decay channels. We identify dominant topological parameters, determined by available data, allowing us to explain the experimental ratios B(Ωc0→Ξ∗0Kˉ∗0)/B(Ωc0→Ω−ρ+)=0.28±0.11{\cal B}(\Omega_c^0\to\Xi^{*0}\bar K^{*0})/{\cal B}(\Omega_c^0\to\Omega^-\rho^+)=0.28\pm 0.11, B(Ωc0→Ξ−π+)/B(Ωc0→Ξ0Kˉ0)=0.10±0.02{\cal B}(\Omega_c^0\to\Xi^-\pi^+)/{\cal B}(\Omega_c^0\to\Xi^{0}\bar K^{0})=0.10\pm 0.02, and B(Ωc0→Ω−K+)/B(Ωc0→Ω−π+)=0.06±0.01{\cal B}(\Omega_c^0 \to \Omega^- K^+)/{\cal B}(\Omega_c^0 \to \Omega^- \pi^+)=0.06\pm 0.01. We also calculate the branching fractions of the Cabibbo-allowed decays, such as B(Ωc0→Ξ∗0Kˉ0)=(9.8±1.3)×10−4{\cal B}(\Omega_c^0 \to \Xi^{* 0} \bar{K}^{0})=(9.8\pm1.3)\times 10^{-4}. In particular, we establish approximate isospin relations: B(Ωc0→Ξ(∗)−π+)≃2B(Ωc0→Ξ(∗)0π0){\cal B}(\Omega_c^0 \to \Xi^{(*)-} \pi^+)\simeq 2{\cal B}(\Omega_c^0 \to \Xi^{(*)0} \pi^0) and B(Ωc0→Ξ(∗)−ρ+)≃2B(Ωc0→Ξ(∗)0ρ0){\cal B}(\Omega_c^0 \to \Xi^{(*)-} \rho^+)\simeq 2{\cal B}(\Omega_c^0 \to \Xi^{(*)0} \rho^0), where B(Ωc0→Ξ0π0)=(2.3±0.2)×10−4{\cal B}(\Omega_c^0 \to \Xi^0 \pi^0)=(2.3\pm0.2)\times 10^{-4} is accessible to the Belle and LHCb experiments.Comment: 16 pages, 3 tables, 2 figure

    A Study on Knowledge Sharing in Vietnamese Organizations

    Get PDF
    Knowledge sharing is very much a sign for the atmosphere of social interactions in the organizations, it depends on the quality of the conversation, formally or informally. In other words, for more effective knowledge sharing, communication competence is required in order to have appropriate conversation. During the past decades, most theories of communication competence have been developed on the basis of “western” conceptualization. This empirical research is conducted in order to study the organizational communication competence in a non-western country, Vietnam, and the effect of such competence to the employees’ knowledge sharing behavior respectively. Base on the data collected from 11 organizations, the effects of three culture dimensions, namely individualism, power distance, and uncertainty avoidance to the communication competence were statistically analyzed; then, stemming from the certain level of communication competence, the behavior of organizational members towards knowledge sharing was explaine

    Probing the ISM Near Star Forming Regions with GRB Afterglow Spectroscopy: Gas, Metals, and Dust

    Full text link
    We study the chemical abundances of the interstellar medium surrounding high z gamma-ray bursts (GRBs) through analysis of the damped Lya systems (DLAs) identified in afterglow spectra. These GRB-DLAs are characterized by large HI column densities N(HI) and metallicities [M/H] spanning 1/100 to nearly solar, with median [M/H]>-1. The majority of GRB-DLAs have [M/H] values exceeding the cosmic mean metallicity of atomic gas at z>2, i.e. if anything, the GRB-DLAs are biased to larger metallicity. We also observe (i) large [Zn/Fe] values (>+0.6) and sub-solar Ti/Fe ratios which imply substantial differential depletion, (ii) large a/Fe ratios suggesting nucleosynthetic enrichment by massive stars, and (iii) low C^0/C^+ ratios (<10^{-4}). Quantitatively, the observed depletion levels and C^0/C^+ ratios of the gas are not characteristic of cold, dense HI clouds in the Galactic ISM. We argue that the GRB-DLAs represent the ISM near the GRB but not gas directly local to the GRB (e.g. its molecular cloud or circumstellar material). We compare these observations with DLAs intervening background quasars (QSO-DLAs). The GRB-DLAs exhibit larger N(HI) values, higher a/Fe and Zn/Fe ratios, and have higher metallicity than the QSO-DLAs. We argue that the differences primarily result from galactocentric radius-dependent differences in the ISM: GRB-DLAs preferentially probe denser, more depleted, higher metallicity gaslocated in the inner few kpc whereas QSO-DLAs are more likely to intersect the less dense, less enriched, outer regions of the galaxy. Finally, we investigate whether dust obscuration may exclude GRB-DLA sightlines from QSO-DLA samples; we find that the majority of GRB-DLAs would be recovered which implies little observational bias against large N(HI) systems.Comment: 16 pages, 9 figures. Submitted to Ap

    Critical behavior of the 3-state Potts model on Sierpinski carpet

    Full text link
    We study the critical behavior of the 3-state Potts model, where the spins are located at the centers of the occupied squares of the deterministic Sierpinski carpet. A finite-size scaling analysis is performed from Monte Carlo simulations, for a Hausdorff dimension dfd_{f} ≃1.8928\simeq 1.8928. The phase transition is shown to be a second order one. The maxima of the susceptibility of the order parameter follow a power law in a very reliable way, which enables us to calculate the ratio of the exponents Îł/Îœ\gamma /\nu. We find that the scaling corrections affect the behavior of most of the thermodynamical quantities. However, the sequence of intersection points extracted from the Binder's cumulant provides bounds for the critical temperature. We are able to give the bounds for the exponent 1/Îœ1/\nu as well as for the ratio of the exponents ÎČ/Îœ\beta/\nu, which are compatible with the results calculated from the hyperscaling relation.Comment: 13 pages, 4 figure
    • 

    corecore