28,808 research outputs found

    The radiative decays of 0++0^{++} and 1+1^{+-} heavy mesons

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    The radiative decay is believed to be an ideal lab to study hadronic structure of newly observed resonances because the reactions are governed by only the electromagnetic interaction (tree level). However, to obtain correct theoretical values, one has to properly deal with the non-perturbative QCD effects in the wavefunction and hadronization. In this work we derive the formulas for the radiative decays of 0++0^{++} and 1+1^{-+} heavy mesons in the light front quark model (LFQM). Because B(χc0J/ψγ)\mathcal{B}(\chi_{c0}\rightarrow J/\psi\gamma) is well measured, the theoretical evaluation of the transition rate can be used to test our approach. Within this theoretical framework, the width of χb0Υ(1S)γ\chi_{b0}\rightarrow \Upsilon(1S)\gamma is evaluated. The formulas can be applied to identify the inner structures of new resonances, for example the isospin of hc(b)h_{c(b)} and the structure of Ds(2317)D_s(2317), via processes hcηcγh_c\rightarrow \eta_c\gamma, hbηbγh_b\rightarrow \eta_b\gamma and Ds(2317)Ds+γD_s(2317)\rightarrow D_s^*+\gamma.Comment: 10 pages, 1 figure, Accepted by PR

    A comparison of different cluster mass estimates: consistency or discrepancy ?

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    Rich and massive clusters of galaxies at intermediate redshift are capable of magnifying and distorting the images of background galaxies. A comparison of different mass estimators among these clusters can provide useful information about the distribution and composition of cluster matter and their dynamical evolution. Using a hitherto largest sample of lensing clusters drawn from literature, we compare the gravitating masses of clusters derived from the strong/weak gravitational lensing phenomena, from the X-ray measurements based on the assumption of hydrostatic equilibrium, and from the conventional isothermal sphere model for the dark matter profile characterized by the velocity dispersion and core radius of galaxy distributions in clusters. While there is an excellent agreement between the weak lensing, X-ray and isothermal sphere model determined cluster masses, these methods are likely to underestimate the gravitating masses enclosed within the central cores of clusters by a factor of 2--4 as compared with the strong lensing results. Such a mass discrepancy has probably arisen from the inappropriate applications of the weak lensing technique and the hydrostatic equilibrium hypothesis to the central regions of clusters as well as an unreasonably large core radius for both luminous and dark matter profiles. Nevertheless, it is pointed out that these cluster mass estimators may be safely applied on scales greater than the core sizes. Namely, the overall clusters of galaxies at intermediate redshift can still be regarded as the dynamically relaxed systems, in which the velocity dispersion of galaxies and the temperature of X-ray emitting gas are good indicators of the underlying gravitational potentials of clusters.Comment: 16 pages with 7 PS figures, MNRAS in pres

    Cosmological constraint on Brans-Dicke Model

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    We combine new Cosmic Microwave Background (CMB) data from Planck with Baryon Acoustic Oscillation (BAO) data to constrain the Brans-Dicke (BD) theory, in which the gravitational constant GG evolves with time. Observations of type Ia supernovae (SNeIa) provide another important set of cosmological data, as they may be regarded as standard candles after some empirical corrections. However, in theories that include modified gravity like the BD theory, there is some risk and complication when using the SNIa data because their luminosity may depend on GG. In this paper, we assume a power law relation between the SNIa luminosity and GG, but treat the power index as a free parameter. We then test whether the difference in distances measured with SNIa data and BAO data can be reduced in such a model. We also constrain the BD theory and cosmological parameters by making a global fit with the CMB, BAO and SNIa data set. For the CMB+BAO+SNIa data set, we find 0.08×102<ζ<0.33×1020.08\times10^{-2} < \zeta <0.33\times10^{-2} at the 68\% confidence level (CL) and 0.01×102<ζ<0.43×102-0.01\times10^{-2} <\zeta <0.43\times 10^{-2} at the 95\% CL, where ζ\zeta is related to the {BD} parameter ω\omega by ζ=ln(1+1/ω)\zeta=\ln(1+1/\omega).Comment: 13pages, 7 figures, to appear on RA

    The Oblique Corrections from Heavy Scalars in Irreducible Representations

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    The contributions to SS, TT, and UU from heavy scalars in any irreducible representation of the electroweak gauge group SU(2)L×U(1)YSU(2)_L\times U(1)_Y are obtained. We find that in the case of a heavy scalar doublet there is a slight difference between the SS parameter we have obtained and that in previous works.Comment: 6 pages, 2 axodraw figures; minor changes, references update

    Is Zb(10610)Z_b(10610) a Molecular State?

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    Whether molecular states indeed exist in nature has been disputed for a long time. Several new resonances have been observed in the recent experiments and they seem to be of exotic structures and some of them have been proposed to be molecular states. The very recent observation of Zb(10610)[(10608.4±2.0)Z_b(10610)[(10608.4\pm 2.0) MeV] and Zb(10650)[(10653.2±1.5)Z_b(10650)[(10653.2\pm 1.5) MeV] encourages the interpretation of multi-quark states. In the Beter-Salpeter (BS) approach, we study the possibility if two heavy mesons can form a molecular state by exchanging light mesons. Our results indicate that two heavy mesons can form an isospin singlet (I=0) bound state but cannot form an isospin triplet (I=1) when the contribution of σ\sigma- exchange is reasonably small, i.e. as the coupling of σ\sigma with mesons gσg_{\sigma} takes the value given in previous literatures. Thus we conclude that the newly observed Zb(10610)Z_b(10610) should not be a molecular state, but a tetraquark state instead, at most, the fraction of the molecular state in the physical resonance Zb(10610)Z_b(10610) is tiny.Comment: 15 pages, 2 figures, an important reference added; Accepted by JHE
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