2,573 research outputs found

    A mutation in the interferon regulatory element of HBV may influence the response of interferon treatment in chronic hepatitis B patients

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    <p>Abstract</p> <p>Background</p> <p>A functional interferon regulatory element (IRE) has been found in the EnhI/X promoter region of hepatitis B virus (HBV) genome. The purpose of this study is to compare the gene order of responder and non-responder to interferon therapy in patients with chronic hepatitis B (CHB), so as to evaluate the relationship between IRE mutation and the response to interferon treatment for CHB patients.</p> <p>Results</p> <p>Synthetic therapeutic effect is divided into complete response (CR), partial response (PR) and non-response (NR). Among the 62 cases included in this study, 40 cases (64.5%) were in the response group (CR and PR) and 22 (35.5%) cases were in the NR group. Wild type sequence of HBV IRE TTTCACTTTC were found in 35 cases (56.5%), and five different IRE gene sequences. included TTTtACTTTC, TTTCAtTTTC, TTTtAtTTTC, TTTtACTTTt and cTTtACcTTC, were found in 22 cases (35.5%), 1 case (1.6%), 1 case (1.6%), 2 cases (3.2%) and 1 case (1.6%) respectively. There were 41.9%cases (26/62) with forth base C→T mutation, consisted of 32.5% (13/40) cases in response group and 59.1% (13/22) cases in NR group. Among the 35 cases with IRE sequences, there were 67.5% (27/40) cases in response group and 36.4% (8/22) in NR group, and the difference in IRE sequences between two groups was statistic significantly (P = 0.027). The result suggested that there is likely relationship between the forth base mutation (C→T) of IRE region and the response of HBV to Interferon therapy, and this mutation may partially decrease the inhibition effect of interferon on HBV.</p> <p>Conclusion</p> <p>The forth base C→T mutation in IRE element of HBV may partially influence the response of Interferon treatment in CHB patients.</p

    The Bˉs0J/ψπ0η\bar B_s^0 \to J/\psi \pi^0 \eta decay and the a0(980)f0(980)a_0(980)-f_0(980) mixing

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    We study the Bˉs0J/ψf0(980)\bar B_s^0 \to J/\psi f_0(980) and Bˉs0J/ψa0(980)\bar B_s^0 \to J/\psi a_0(980) reactions, and pay attention to the different sources of isospin violation and mixing of f0(980)f_0(980) and a0(980)a_0(980) resonances where these resonances are dynamically generated from meson-meson interaction. We find that the main reason of isospin violation is the isospin breaking in the meson-meson transition TT matrices, and the other source is that the loops involving kaons in the production mechanism provide a source of isospin violation because they do not cancel by the different mass of the charged and neutral kaons. We obtain a branching ratio for a0(980)a_0(980) production of the order of 5×1065 \times 10^{-6}. Future experiments can address this problem and the production rate and shape of the π0η\pi^0 \eta mass distribution will definitely help to better understand the nature of scalar resonances.Comment: 12 pages, 4 figure

    4-(4-Bromo­phen­yl)-2,6-diphenyl­pyridine

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    In the title compound, C23H16BrN, the three benzene rings show a disrotatory counter-rotating arrangement around the central pyridine ring and are twisted with respect to the pyridine ring with dihedral angles of 19.56 (13), 27.54 (13) and 30.51 (13)°

    Implementing universal nonadiabatic holonomic quantum gates with transmons

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    Geometric phases are well known to be noise-resilient in quantum evolutions/operations. Holonomic quantum gates provide us with a robust way towards universal quantum computation, as these quantum gates are actually induced by nonabelian geometric phases. Here we propose and elaborate how to efficiently implement universal nonadiabatic holonomic quantum gates on simpler superconducting circuits, with a single transmon serving as a qubit. In our proposal, an arbitrary single-qubit holonomic gate can be realized in a single-loop scenario, by varying the amplitudes and phase difference of two microwave fields resonantly coupled to a transmon, while nontrivial two-qubit holonomic gates may be generated with a transmission-line resonator being simultaneously coupled to the two target transmons in an effective resonant way. Moreover, our scenario may readily be scaled up to a two-dimensional lattice configuration, which is able to support large scalable quantum computation, paving the way for practically implementing universal nonadiabatic holonomic quantum computation with superconducting circuits.Comment: v3 Appendix added, v4 published version, v5 published version with correction
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