4,348 research outputs found

    On the four-zero texture of quark mass matrices and its stability

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    We carry out a new study of quark mass matrices MuM^{}_{\rm u} (up-type) and MdM^{}_{\rm d} (down-type) which are Hermitian and have four zero entries, and find a new part of the parameter space which was missed in the previous works. We identify two more specific four-zero patterns of MuM^{}_{\rm u} and MdM^{}_{\rm d} with fewer free parameters, and present two toy flavor-symmetry models which can help realize such special and interesting quark flavor structures. We also show that the texture zeros of MuM^{}_{\rm u} and MdM^{}_{\rm d} are essentially stable against the evolution of energy scales in an analytical way by using the one-loop renormalization-group equations.Comment: 33 pages, 4 figures, minor comments added, version to appear in Nucl. Phys.

    The longlived charged massive scalar field in the higher-dimensional Reissner--Nordstr\"{o}m spacetime

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    The quasinormal resonance frequency of the higher-dimensional Reissner--Nordstr\"{o}m (RN) black hole due to charged massive scalar field perturbation is deduced analytically in the eikonal regime. The characteristic decay timescale of the charged massive scalar perturbation in the background of the higher-dimensional RN spacetime is then obtained. The result reveals that longlived charged massive scalar field can exist in higher-dimensional RN spacetime under a certain condition.Comment: 6 pages, 1 figur

    Nucleation of membrane adhesions

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    Recent experimental and theoretical studies of biomimetic membrane adhesions [Bruinsma et al., Phys. Rev. E 61, 4253 (2000); Boulbitch et al., Biophys. J. 81, 2743 (2001)] suggested that adhesion mediated by receptor interactions is due to the interplay between membrane undulations and a double-well adhesion potential, and should be a first-order transition. We study the nucleation of membrane adhesion by finding the minimum-energy path on the free energy surface constructed from the bending free energy of the membrane and the double-well adhesion potential. We find a nucleation free energy barrier around 20kBT for adhesion of flexible membranes, which corresponds to fast nucleation kinetics with a time scale of the order of seconds. For cell membranes with a larger bending rigidity due to the actin network, the nucleation barrier is higher and may require active processes such as the reorganization of the cortex network to overcome this barrier. Our scaling analysis suggests that the geometry of the membrane shapes of the adhesion contact is controlled by the adhesion length that is determined by the membrane rigidity, the barrier height, and the length scale of the double-well potential, while the energetics of adhesion is determined by the depths of the adhesion potential. These results are verified by numerical calculations

    The effective neutrino mass of neutrinoless double-beta decays: how possible to fall into a well

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    If massive neutrinos are the Majorana particles and have a normal mass ordering, the effective mass term ⟨m⟩ee\langle m\rangle^{}_{ee} of a neutrinoless double-beta (0Ξ½2Ξ²0\nu 2\beta) decay may suffer significant cancellations among its three components and thus sink into a decline, resulting in a "well" in the three-dimensional graph of ∣⟨m⟩ee∣|\langle m\rangle^{}_{ee}| against the smallest neutrino mass m1m^{}_1 and the relevant Majorana phase ρ\rho. We present a new and complete analytical understanding of the fine issues inside such a well, and discover a novel threshold of ∣⟨m⟩ee∣|\langle m\rangle^{}_{ee}| in terms of the neutrino masses and flavor mixing angles: ∣⟨m⟩eeβˆ£βˆ—=m3sin⁑2ΞΈ13|\langle m\rangle^{}_{ee}|^{}_* = m^{}_3 \sin^2\theta^{}_{13} in connection with tan⁑θ12=m1/m2\tan\theta^{}_{12} = \sqrt{m^{}_1/m^{}_2} and ρ=Ο€\rho =\pi. This threshold point, which links the {\it local} minimum and maximum of ∣⟨m⟩ee∣|\langle m\rangle^{}_{ee}|, can be used to signify observability or sensitivity of the future 0Ξ½2Ξ²0\nu 2\beta-decay experiments. Given current neutrino oscillation data, the possibility of ∣⟨m⟩ee∣<∣⟨m⟩eeβˆ£βˆ—|\langle m\rangle^{}_{ee}| < |\langle m\rangle^{}_{ee}|^{}_* is found to be very small.Comment: 9 pages, 3 figures, version to appear in Eur. Phys. J.
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