394 research outputs found

    The Study on RFID Security Method for Entrance Guard System

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    The RFID technology has been used by industries in recent years, for examples, replacing the traditional two-dimensional barcode, logistics management, military applications, identification. In fact, RFID technology has become one of the new killer technologies. The RFID uses radio frequency to convey information which involves, however, many security problems; Current RFID guidelines do not present solutions to these security problems. The methods put forward in published paper fail to offer complete solutions, either. This study identifies RFID security method for Entrance Guard system. The algorithms used include Hash, AES, random values, XOR four item technology, and use the three-way authentication structure to solve the safety problems of the certification of Entrance Guard system. The experiment showed the algorithms provided better protection on the current RFID systems against attack methods such as Eavesdropping, Traceability, Spoofing and Replay attacking

    Perturbative QCD analysis of B→ϕK∗B \to \phi K^* decays

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    We study the first observed charmless B→VVB\to VV modes, the B→ϕK∗B\to\phi K^* decays, in perturbative QCD formalism. The obtained branching ratios B(B→ϕK∗)∌15×10−6B(B\to\phi K^*)\sim 15 \times 10^{-6} are larger than ∌9×10−6\sim 9\times 10^{-6} from QCD factorization. The comparison of the predicted magnitudes and phases of the different helicity amplitudes, and branching ratios with experimental data can test the power counting rules, the evaluation of annihilation contributions, and the mechanism of dynamical penguin enhancement in perturbative QCD, respectively.Comment: 14 pages, 2 tables, brief disscussion on hard sacle added, version to appear in PR

    Graphite felt with vapor grown carbon fibers as electrodes for vanadium redox flow batteries

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    Several methods to produce vapor grown carbon fibers (VGCFs) on graphite felt as electrodes for vanadium redox flow batteries (VRB) were described. The experiments include graphite felt preparation and VGCF production onto graphite fiber in the felt. Several attempts were made using nickel and cobalt catalyst coatings on the graphite felt. The nickel catalyst came from nickel nitride solution. It was prepared by dipping graphite felt into the solution and decomposed using heat treatment. Cobalt nanoparticles were sprayed onto graphite felt. Both experiments resulted in carbon nanotubes and VGCFs growth onto graphite fiber in the felt. The experimental results show that VGCFs and carbon nanotubes with the range of 20 to 70 nm in diameter are grown in the graphite felt using different catalysts. The encouraged results show the single VRB cell test with new electrodes can increase the charge/discharge efficiency by more than 12% compared to conventional graphite felt

    Evidence for two-quark content of f0(980)f_{0}(980) in exclusive b→cb\to c decays

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    Inspired by a large decay branching ratio (BR) of B+→f0(980)K+B^{+}\to f_{0}(980)K^{+} measured by Belle recently, we propose that a significant evidence of the component of nnˉ=(uuˉ+ddˉ)/2n\bar{n}=(u\bar{u}+d\bar{d})/\sqrt{2} in f0(980)f_{0}(980) could be demonstrated in exclusive b→cb\to c decays by the observation of f0(980)f_{0}(980) in the final states Bˉ→D0(∗)π+π−(KK)\bar{B}\to D^{0(*)} \pi^{+} \pi^{-}(KK) and Bˉ→J/Κπ+π−(KK)\bar{B}\to J/\Psi \pi^{+} \pi^{-}(KK). We predict the BRs of Bˉ→D0(∗)(J/Κ)f0(980)\bar{B}\to D^{0(*)} (J/\Psi) f_{0}(980) to be O(10−4){\cal {O}}(10^{-4}) (O(10−5){\cal {O}}(10^{-5})) while the unknown wave functions of D(∗)0D^{(*)0} (J/ΚJ/\Psi) are chosen to fit the observed decays of Bˉ→D(∗)0π0(J/ΚK0(∗))\bar{B}\to D^{(*)0} \pi^{0} (J/\Psi K^{0(*)}).Comment: 4 pages, 2 figures, Revtex4, version to appear in PR

    Cyclin D1 acts as a barrier to pluripotent reprogramming by promoting neural progenitor fate commitment

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    AbstractA short G1 phase is a characteristic feature of the cell cycle structure of pluripotent cells, and is reestablished during Yamanaka factor-mediated pluripotent reprogramming. How cell cycle control is adjusted to meet the requirements of pluripotent cell fate commitment during reprogramming is less well understood. Elevated levels of cyclin D1 were initially found to impair pluripotency maintenance. The current work further identified Cyclin D1 to be capable of transcriptionally upregulating Pax6, which promoted reprogramming cells to commit to a neural progenitor fate rather than a pluripotent cell fate. These findings explain the importance of reestablishment of G1-phase restriction in pluripotent reprogramming

    B→f0(980)K(∗)B\to f_{0}(980) K^{(*)} decays and final state interactions

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    We study the exclusive decays of B→f0(980)K(∗)B\to f_{0}(980) K^{(*)} in the framework of the perturbative QCD by identifying the f0(980)f_{0}(980) as the composition of sˉs\bar{s} s and nˉn=(uˉu+dˉd)/2\bar{n}n=(\bar{u}u+\bar{d}d)/\sqrt{2}. We find that the influence of the nˉn\bar{n} n content on the predicted branching ratios is crucial. We discuss the possible rescattering and gluonium states which could enhance the branching ratios of considered decays. We point out that the CP asymmetry in B→f0(980)KS,LB\to f_{0}(980) K_{S,L} could be a new explorer of sin⁥2ϕ1\sin2\phi_{1}.Comment: 13 pages, 2 figures, Revtex4, final version to appear in Phys. Rev.

    Study of B→D∗∗πB\to D^{**} \pi decays

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    We investigate the production of the novel PP-wave mesons D0∗D^{*}_{0} and D1â€Č(D1)D^{\prime}_{1} (D_{1}), identified as JP=0+J^{P}=0^+ and 1+1^+, in heavy BB meson decays, respectively. With the heavy quark limit, we give our modelling wave functions for the scalar meson D0∗D^{*}_{0}. Based on the assumptions of color transparency and factorization theorem, we estimate the branching ratios of B→D0∗πB\to D^{*}_{0} \pi decays in terms of the obtained wave functions. Some remarks on D1(â€Č)D^{(\prime)}_{1} productions are also presented.Comment: 16 pages, 2 figures, Revtex4, to be published in Phys. Rev.

    Applicability of perturbative QCD to Λb→Λc\Lambda_b \to \Lambda_c decays

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    We develop perturbative QCD factorization theorem for the semileptonic heavy baryon decay Λb→ΛclΜˉ\Lambda_b \to \Lambda_c l\bar{\nu}, whose form factors are expressed as the convolutions of hard bb quark decay amplitudes with universal Λb\Lambda_b and Λc\Lambda_c baryon wave functions. Large logarithmic corrections are organized to all orders by the Sudakov resummation, which renders perturbative expansions more reliable. It is observed that perturbative QCD is applicable to Λb→Λc\Lambda_b \to \Lambda_c decays for velocity transfer greater than 1.2. Under requirement of heavy quark symmetry, we predict the branching ratio B(Λb→ΛclΜˉ)∌2B(\Lambda_b \to \Lambda_c l{\bar\nu})\sim 2%, and determine the Λb\Lambda_b and Λc\Lambda_c baryon wave functions.Comment: 12 pages in Latex file, 3 figures in postscript files, some results are changed, but the conclusion is the sam

    Final state interaction and B→KKB\to KK decays in perturbative QCD

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    We predict branching ratios and CP asymmetries of the B→KKB\to KK decays using perturbative QCD factorization theorem, in which tree, penguin, and annihilation contributions, including both factorizable and nonfactorizable ones, are expressed as convolutions of hard six-quark amplitudes with universal meson wave functions. The unitarity angle ϕ3=90o\phi_3= 90^o and the BB and KK meson wave functions extracted from experimental data of the B→KπB\to K\pi and ππ\pi\pi decays are employed. Since the B→KKB\to KK decays are sensitive to final-state-interaction effects, the comparision of our predictions with future data can test the neglect of these effects in the above formalism. The CP asymmetry in the B±→K±K0B^\pm\to K^\pm K^0 modes and the Bd0→K±K∓B_d^0\to K^\pm K^\mp branching ratios depend on annihilation and nonfactorizable amplitudes. The B→KKB\to KK data can also verify the evaluation of these contributions.Comment: 13 pages in latex file, 7 figures in ps file

    Forced flowering of pineapple (Ananas comosus cv. Tainon 17) in response to cold stress, ethephon and calcium carbide with or without activated charcoal

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    Ethylene, a gaseous plant hormone, is responsible for the initiation of reproductive development in pineapple. Reproductive development can be forced in pineapple (Ananas comosus var. comosus) throughout the year with ethylene. Inhibition of natural flowering initiation with aviglycine [(S)-trans-2-amino-4-(2-aminoethoxy)-3-butenoic acid hydrochloride], an inhibitor of ethylene biosynthesis, provides evidence that reproductive development in response to cold stress and short daylength is also in response to ethylene production. We studied the effect of cold treatment of pineapple on ethylene production and flower induction by applying a short-term cold stress to stem apices. Shoot apices of pineapple treated with ice crystals also produced twice as much ethylene as did those of control plants and significantly more than was produced by "D" leaf basal tissue. Moreover, pineapple plants treated four times with ice crystals or ice water were induced to flower under field conditions and the forcing efficiency, as evaluated by the percentages of inflorescence emergence and fruit harvest, was comparable to forcing with calcium carbide (CaC(2)) and ethephon. In another field experiment two applications of a 1.0% solution of CaC(2) or 0.15% ethephon applied at 48 h intervals was sufficient to force reproductive development of 'Tainon 17'. Furthermore, 0.5 or 1.0% solutions of CaC(2) supplemented with 0.5% activated charcoal (AC) significantly improved the forcing effectiveness of CaC(2). This could/would make it possible to reduce the number or concentration, or both, of CaC(2) required to effect forcing in pineapple
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