20,517 research outputs found

    B_{s1}(5830) and B_{s2}^*(5840)

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    In this paper we investigate the strong decays of the two newly observed bottom-strange mesons Bs1(5830)B_{s1}(5830) and Bs2(5840)B_{s2}^*(5840) in the framework of the quark pair creation model. The two-body strong decay widths of Bs1(5830)0B+KB_{s1}(5830)^0\to B^{*+}K^- and Bs2(5840)0B+K,B+KB_{s2}^*(5840)^0\to B^+K^-, B^{*+}K^- are calculated by considering Bs1(5830)B_{s1}(5830) to be a mixture between 1P1>|^1P_1> and 3P1>|^3P_1> states, and Bs2(5840)B_{s2}^*(5840) to be a 3P2>|^3P_2> state. The double pion decay of Bs1(5830)B_{s1}(5830) and Bs2(5840)B_{s2}^*(5840) is supposed to occur via the intermediate state σ\sigma and f0(980)f_0(980). Although the double pion decay widths of Bs1(5830)B_{s1}(5830) and Bs2(5840)B_{s2}^*(5840) are smaller than the two-body strong decay widths of Bs1(5830)B_{s1}(5830) and Bs2(5840)B_{s2}^*(5840), one suggests future experiments to search the double pion decays of Bs1(5830)B_{s1}(5830) and Bs2(5840)B_{s2}^*(5840) due to their sizable decay widths.Comment: 9 pages, 8 figures and 6 tables. More references and discussions added, typos corrected, some descriptions changed. Publication version in PR

    Production of Charmed Tetraquarks from BcB_c and BB decays

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    Hadronic states composed of multi-quark flavors may exist in reality since they are not prohibited by QCD. Compact four quark systems of color singlet are classified as tetraquarks. To understand the properties of these states, more theoretical and experimental efforts are needed. In this work, we study charmed tetraquarks with three light flavors using flavor SU(3)SU(3) symmetry. States with three different light quarks must be in a 6ˉ{\bf \bar 6 } or a 15{\bf 15} multiplet. We investigate the production of charmed tetraquarks XcX_c in BXc(Xc)PB\to X_c (\overline {X}_c) P and BcXcPB_c \to X_c P decays. Whether the states with three light quarks belong to 6ˉ{\bf \bar 6} or 15{\bf 15} can be determined by studying various tetraquark BB and BcB_c decays. We demonstrate that the decay amplitudes for these decays can be parametrized by a few irreducible SU(3) invariant amplitudes. We then derive relations for decay widths and CP violating rate difference which can be examined experimentally. Although no experimental measurement is available yet, they might be accessed at the ongoing and forthcoming experiments like the LHCb and Belle-II. Measurements of these observables can not only provide useful information for the study of exotics spectroscopy but are also valuable information towards a better understanding of some non-perturbative aspects of QCD.Comment: 14 page

    A Revisit to Quadratic Programming with One Inequality Quadratic Constraint via Matrix Pencil

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    The quadratic programming over one inequality quadratic constraint (QP1QC) is a very special case of quadratically constrained quadratic programming (QCQP) and attracted much attention since early 1990's. It is now understood that, under the primal Slater condition, (QP1QC) has a tight SDP relaxation (PSDP). The optimal solution to (QP1QC), if exists, can be obtained by a matrix rank one decomposition of the optimal matrix X? to (PSDP). In this paper, we pay a revisit to (QP1QC) by analyzing the associated matrix pencil of two symmetric real matrices A and B, the former matrix of which defines the quadratic term of the objective function whereas the latter for the constraint. We focus on the \undesired" (QP1QC) problems which are often ignored in typical literature: either there exists no Slater point, or (QP1QC) is unbounded below, or (QP1QC) is bounded below but unattainable. Our analysis is conducted with the help of the matrix pencil, not only for checking whether the undesired cases do happen, but also for an alternative way to compute the optimal solution in comparison with the usual SDP/rank-one-decomposition procedure.Comment: 22 pages, 0 figure

    Drive laser system for the DC-SRF photoinjector at Peking University

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    Photoinjectors are widely used for linear accelerators as electron sources to generate high-brightness electron beam. Drive laser, which determines the timing structure and quality of the electron beam, is a crucial device of photoinjector. A new drive laser system has been designed and constructed for the upgraded 3.5-cell DC-SRF photoinjector at Peking University. The drive laser system consists of a 1064 nm laser oscillator, a four- stage amplifier, the second and fourth harmonic generators, the optical system to transfer the UV pulses to the photocathode, and the synchronization system. The drive laser system has been successfully applied in the stable operation of DC-SRF photoinjector and its performance meets the requirements. 266 nm laser with an average power close to 1W can be delivered to illuminate the Cs2Te photocathode and the instability is less than 5% for long time operation. The design consideration for improving the UV laser quality, a detailed description of laser system, and its performance are presented in this paper.Comment: 6 pages, 8 figures, submit to CP

    Deflationary Expansion : an Overshooting Perspective to the Recent Business Cycle in China

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    Deflationary expansion has puzzled economists both in and outside China. We study this business cycles phenomenon within a model of discrete time dynamics. We find that deflationary expansion could be possible if driven by an overshooting in investing and if the state of the economy maintains high rate of growth. This expression is consistent with the recent variables. The high steady state of growth could be explained by the current institutional environment of China.Deflationary Expansion, China, Existence and Stability Conditions of Equilibrium, Business Fluctuations, monetary policy, Central Banking, Supply of Money and Credit
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