12,801 research outputs found

    Some Predictions of Diquark Model for Hidden Charm Pentaquark Discovered at the LHCb

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    The LHCb has discovered two new states with preferred JPJ^P quantum numbers 3/2−3/2^- and 5/2+5/2^+ from Λb\Lambda_b decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these pentaquarks can be described by diquark model. The diquark model predicts that the 3/2−3/2^- and 5/2+5/2^+ are in two separate octet multiplets of flavor SU(3)SU(3) and there is also an additional decuplet pentaquark multiplet. Finding the states in these multiplets can provide crucial evidence for this model. The weak decays of b-baryon to a light meson and a pentaquark can have Cabibbo allowed and suppressed decay channels. We find that in the SU(3)SU(3) limit, for UU-spin related decay modes the ratio of the decay rates of Cabibbo suppressed to Cabibbo allowed decay channels is given by ∣Vcd∣2/∣Vcs∣2|V_{cd}|^2/|V_{cs}|^2. There are also other testable relations for b-baryon weak decays into a pentaquark and a light pseudoscalar. These relations can be used as tests for the diquark model for pentaquark.Comment: revtex, 19 pages, 3 figures. one reference added and some typos correcte

    Statistical computation of Boltzmann entropy and estimation of the optimal probability density function from statistical sample

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    In this work, we investigate the statistical computation of the Boltzmann entropy of statistical samples. For this purpose, we use both histogram and kernel function to estimate the probability density function of statistical samples. We find that, due to coarse-graining, the entropy is a monotonic increasing function of the bin width for histogram or bandwidth for kernel estimation, which seems to be difficult to select an optimal bin width/bandwidth for computing the entropy. Fortunately, we notice that there exists a minimum of the first derivative of entropy for both histogram and kernel estimation, and this minimum point of the first derivative asymptotically points to the optimal bin width or bandwidth. We have verified these findings by large amounts of numerical experiments. Hence, we suggest that the minimum of the first derivative of entropy be used as a selector for the optimal bin width or bandwidth of density estimation. Moreover, the optimal bandwidth selected by the minimum of the first derivative of entropy is purely data-based, independent of the unknown underlying probability density distribution, which is obviously superior to the existing estimators. Our results are not restricted to one-dimensional, but can also be extended to multivariate cases. It should be emphasized, however, that we do not provide a robust mathematical proof of these findings, and we leave these issues with those who are interested in them.Comment: 8 pages, 6 figures, MNRAS, in the pres

    Collective cell migration: Implications for wound healing and cancer invasion.

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    During embryonic morphogenesis, wound repair and cancer invasion, cells often migrate collectively via tight cell-cell junctions, a process named collective migration. During such migration, cells move as coherent groups, large cell sheets, strands or tubes rather than individually. One unexpected finding regarding collective cell migration is that being a "multicellular structure" enables cells to better respond to chemical and physical cues, when compared with isolated cells. This is important because epithelial cells heal wounds via the migration of large sheets of cells with tight intercellular connections. Recent studies have gained some mechanistic insights that will benefit the clinical understanding of wound healing in general. In this review, we will briefly introduce the role of collective cell migration in wound healing, regeneration and cancer invasion and discuss its underlying mechanisms as well as implications for wound healing

    Search for a heavy dark photon at future e+e−e^+e^- colliders

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    A coupling of a dark photon A′A' from a U(1)A′U(1)_{A'} with the standard model (SM) particles can be generated through kinetic mixing represented by a parameter ϵ\epsilon. A non-zero ϵ\epsilon also induces a mixing between A′A' and ZZ if dark photon mass mA′m_{A'} is not zero. This mixing can be large when mA′m_{A'} is close to mZm_Z even if the parameter ϵ\epsilon is small. Many efforts have been made to constrain the parameter ϵ\epsilon for a low dark photon mass mA′m_{A'} compared with the ZZ boson mass mZm_Z. We study the search for dark photon in e+e−→γA′→γμ+μ−e^+e^- \to \gamma A' \to \gamma \mu^+ \mu^- for a dark photon mass mA′m_{A'} as large as kinematically allowed at future e+e−e^+e^- colliders. For large mA′m_{A'}, care should be taken to properly treat possible large mixing between A′A' and ZZ. We obtain sensitivities to the parameter ϵ\epsilon for a wide range of dark photon mass at planed e+  e−e^+\;e^- colliders, such as Circular Electron Positron Collider (CEPC), International Linear Collider (ILC) and Future Circular Collider (FCC-ee). For the dark photon mass 20 GeV≲mA′≲330 GeV20~\text{GeV}\lesssim m_{A^{\prime}}\lesssim 330~\text{GeV}, the 2σ2\sigma exclusion limits on the mixing parameter are ϵ≲10−3−10−2\epsilon\lesssim 10^{-3}-10^{-2}. The CEPC with s=240 GeV\sqrt{s}=240~\text{GeV} and FCC-ee with s=160 GeV\sqrt{s}=160~\text{GeV} are more sensitive than the constraint from current LHCb measurement once the dark photon mass mA′≳50 GeVm_{A^{\prime}}\gtrsim 50~\text{GeV}. For mA′≳220 GeVm_{A^{\prime}}\gtrsim 220~\text{GeV}, the sensitivity at the FCC-ee with s=350 GeV\sqrt{s}=350~\text{GeV} and 1.5 ab−11.5~\text{ab}^{-1} is better than that at the 13~TeV LHC with 300 fb−1300~\text{fb}^{-1}, while the sensitivity at the CEPC with s=240 GeV\sqrt{s}=240~\text{GeV} and 5 ab−15~\text{ab}^{-1} can be even better than that at 13~TeV LHC with 3 ab−13~\text{ab}^{-1} for mA′≳180 GeVm_{A^{\prime}}\gtrsim 180~\text{GeV}.Comment: 21 pages, 5 figures, 2 table

    Efficiency and power of minimally nonlinear irreversible heat engines with broken time-reversal symmetry

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    We study the minimally nonlinear irreversible heat engines in which the time-reversal symmetry for the systems may b e broken. The expressions for the power and the efficiency are derived, in which the effects of the nonlinear terms due to dissipations are included. We show that, as within the linear responses, the minimally nonlinear irreversible heat engines enable attainment of Carnot efficiency at positive power. We also find that the Curzon-Ahlborn limit imposed on the efficiency at maximum power can be overcomed if the time-reversal symmetry is broken

    Market Stability Switches in a Continuous-Time Financial Market with Heterogeneous Beliefs

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    By considering a financial market of fundamentalists and trend followers in which the price trend of the trend followers is formed as a weighted average of historical prices, we establish a continuous-time financial market model with time delay and examines the impact of time delay on market price dynamics. Conditions for the stability of the fundamental price in terms of agents' behavior parameters and time delay are obtained. In particular, it is found that an increase in time delay can not only destabilize the market price but also stabilize an otherwise unstable market price, leading to stability switching as delay increases. This interesting phenomena shed new light in understanding of mechanism on the market stability. When the fundamental price becomes unstable through Hopf bifurcations, suffcient conditions on the stability and global existence of the periodic solution are obtained.asset price; fundamentalists; trend followers; delay differential equations; stability; bifurcations
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