30,687 research outputs found

    Saddle-point entropy states of equilibrated self-gravitating systems

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    In this Letter, we investigate the stability of the statistical equilibrium of spherically symmetric collisionless self-gravitating systems. By calculating the second variation of the entropy, we find that perturbations of the relevant physical quantities should be classified as long- and short-range perturbations, which correspond to the long- and short-range relaxation mechanisms, respectively. We show that the statistical equilibrium states of self-gravitating systems are neither maximum nor minimum, but complex saddle-point entropy states, and hence differ greatly from the case of ideal gas. Violent relaxation should be divided into two phases. The first phase is the entropy-production phase, while the second phase is the entropy-decreasing phase. We speculate that the second-phase violent relaxation may just be the long-wave Landau damping, which would work together with short-range relaxations to keep the system equilibrated around the saddle-point entropy states.Comment: 5 pages, 1 figure, MNRAS Letter, in the pres

    Perturbative QCD analysis of Dalitz decays J/ψ→η(′)ℓ+ℓ−J/\psi\rightarrow\eta^{(\prime)}\ell^{+}\ell^{-}

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    In the framework of perturbative QCD, we study the Dalitz decays J/ψ→η(′)e+e−J/\psi\rightarrow\eta^{(\prime)}e^{+}e^{-} with large recoil momentum. Meanwhile, the soft contributions from the small recoil momentum region and the VMD corrections have also been taken into account. The transition form factors fψη(′)(q2)f_{\psi\eta^{(\prime)}}(q^{2}) including the hard and soft contributions as well as the VMD corrections are calculated for the first time. By analytical evaluation of the involved one-loop integrals, we find that the transition form factors are insensitive to both the light quark masses and the shapes of η(′)\eta^{(\prime)} distribution amplitudes. With the normalized transition form factors, our results of the branching ratios B(J/ψ→η(′)e+e−)\mathcal{B}(J/\psi\rightarrow\eta^{(\prime)}e^{+}e^{-}) and their ratio RJ/ψe=B(J/ψ→ηe+e−)/B(J/ψ→η′e+e−)R_{J/\psi}^{e}=\mathcal{B}(J/\psi\rightarrow\eta e^{+}e^{-})/\mathcal{B}(J/\psi\rightarrow\eta^{\prime}e^{+}e^{-}) are in good agreement with their experimental data. Furthermore, by the ratio RJ/ψeR_{J/\psi}^{e}, we extract the mixing angle of η−η′\eta-\eta^{\prime} system ϕ=34.0∘±0.6∘\phi=34.0^{\circ}\pm0.6^{\circ} and comment on this result briefly. Inputting the mixing angle ϕ\phi extracted from RJ/ψeR_{J/\psi}^{e}, we predict the branching ratios B(J/ψ→ημ+μ−)=3.64×10−6\mathcal{B}(J/\psi\rightarrow\eta\mu^{+}\mu^{-})=3.64\times10^{-6}, B(J/ψ→η′μ+μ−)=1.52×10−5\mathcal{B}(J/\psi\rightarrow\eta^{\prime}\mu^{+}\mu^{-})=1.52\times10^{-5} and their ratio RJ/ψμ=23.9%R_{J/\psi}^{\mu}=23.9\%.Comment: 14 pages, 9 figures and 5 table

    Twist-3 contributions to γγ→π+π−,K+K−\gamma\gamma\rightarrow\pi^+\pi^-,K^+K^- processes in perturbative QCD approach

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    As one of the simplest hadronic processes, γγ→M+M−\gamma\gamma\rightarrow M^{+}M^{-} (M=π,KM=\pi,K) could be a good testing ground for our understanding of the perturbative and nonperturbative structure of QCD, and will be studied with high precision at BELLE-\RNum{2} in the near future. In this paper, we revisit these processes with twist-3 corrections in the perturbative QCD approach based on the kTk_{T} factorization theorem, in which transverse degrees of freedom as well as resummation effects are taken into account. The influence of the distribution amplitudes on the cross sections are discussed in detail. Our work shows that not only the transverse momentum effects but also the twist-3 corrections play a significant role in the processes γγ→M+M−\gamma\gamma\rightarrow M^{+}M^{-} in the intermediate energy region. Especially in the few GeV region, the twist-3 contributions become dominant in the cross sections. And it is noteworthy that both the twist-3 result of the π+π−\pi^{+}\pi^{-} cross section and that of the K+K−K^{+}K^{-} cross section agree well with the BELLE and ALEPH measurements. For the pion and kaon angular distributions, there still exist discrepancies between our results and the experimental measurements. Possible reasons for these discrepancies are discussed briefly.Comment: 19 pages, 7 figures and 2 tables. Contents improved and more discussions adde
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