281,097 research outputs found

    Deviations of the Lepton Mapping Matrix from the Harrison-Perkins-Scott Form

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    We propose a simple set of hypotheses governing the deviations of the leptonic mapping matrix from the Harrison-Perkins-Scott (HPS) form. These deviations are supposed to arise entirely from a perturbation of the mass matrix in the charged lepton sector. The perturbing matrix is assumed to be purely imaginary (thus maximally TT-violating) and to have a strength in energy scale no greater (but perhaps smaller) than the muon mass. As we shall show, it then follows that the absolute value of the mapping matrix elements pertaining to the tau lepton deviate by no more than O((mμ/mτ)2)3.5×103O((m_\mu/m_\tau)^2) \simeq 3.5 \times 10^{-3} from their HPS values. Assuming that (mμ/mτ)2(m_\mu/m_\tau)^2 can be neglected, we derive two simple constraints on the four parameters θ12\theta_{12}, θ23\theta_{23}, θ31\theta_{31}, and δ\delta of the mapping matrix. These constraints are independent of the details of the imaginary TT-violating perturbation of the charged lepton mass matrix. We also show that the ee and μ\mu parts of the mapping matrix have a definite form governed by two parameters α\alpha and β\beta; any deviation of order mμ/mτm_\mu/m_\tau can be accommodated by adjusting these two parameters.Comment: 31 pages, 2 figure

    Jarlskog Invariant of the Neutrino Mapping Matrix

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    The Jarlskog Invariant JνmapJ_{\nu-map} of the neutrino mapping matrix is calculated based on a phenomenological model which relates the smallness of light lepton masses mem_e and m1m_1 (of ν1\nu_1) with the smallness of TT violation. For small TT violating phase χl\chi_l in the lepton sector, JνmapJ_{\nu-map} is proportional to χl\chi_l, but mem_e and m1m_1 are proportional to χl2\chi_l^2. This leads to Jνmap1/6memμ+O(memμmτ2)+O(m1m2m32) J_{\nu-map} \cong {1/6}\sqrt{\frac{m_e}{m_\mu}}+O \bigg(\sqrt{\frac{m_em_\mu}{m_\tau^2}}\bigg)+O \bigg(\sqrt{\frac{m_1m_2}{m_3^2}}\bigg). Assuming m1m2m32<<memμ\sqrt{\frac{m_1m_2}{m_3^2}}<<\sqrt{\frac{m_e}{m_\mu}}, we find Jνmap1.16×102J_{\nu-map}\cong 1.16\times 10^{-2}, consistent with the present experimental data.Comment: 19 page

    Shuttle system ascent aerodynamic and plume heating

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    The shuttle program provided a challenge to the aerothermodynamicist due to the complexity of the flow field around the vehicle during ascent, since the configuration causes multiple shock interactions between the elements. Wind tunnel tests provided data for the prediction of the ascent design heating environment which involves both plume and aerodynamic heating phenomena. The approach for the heating methodology based on ground test firings and the use of the wind tunnel data to formulate the math models is discussed

    Dark matter and dark gauge fields

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    Following the unexpected theoretical discovery of a mass dimension one fermionic quantum field of spin one half, we now present first results on two _local_ versions. The Dirac and Majorana fields of the standard model of particle physics are supplemented by their natural counterparts in the dark matter sector. The possibility that a mass dimension transmuting symmetry may underlie a new standard model of particle physics is briefly suggested.Comment: This manuscript combines a plenary talk (by DVA) and an invited talk (by DS) at "Dark 2007 - Sixth International Heidelberg Conference on Dark Matter in Astro and Particle Physics (Sydney, Australia, 24th-28th September 2007)." 11 pages. v2: minor typos correcte

    Bistatic image processing for a 32 x 19 inch model aircraft using scattered fields obtained in the OSU-ESL compact range

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    Inverse Synthetic Aperture Radar (ISAR) images for a 32 in long and 19 in wide model aircraft are documented. Both backscattered and bistatic scattered fields of this model aircraft were measured in the OSU-ESL compact range to obtain these images. The scattered fields of the target were measured for frequencies from 2 to 18 GHz with a 10 MHz increment and for full 360 deg azimuth rotation angles with a 0.2 deg step. For the bistatic scattering measurement, the compact range was used as the transmitting antenna; while, a broad band AEL double ridge horn was used as the receiving antenna. Bistatic angles of 90 deg and 135 deg were measured. Due to the size of the chamber and target, the receiving antenna was in the near field of the target; nevertheless, the image processing algorithm was valid for this case

    Neutron Electric Dipole Moment at Fixed Topology

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    We describe the finite volume effects of CP-odd quantities, such as the neutron electric dipole moment and the anapole moment in the θ\theta-vacuum, under different topological sectors. We evaluate the three-point Green's functions for the electromagnetic current in a fixed non-trivial topological sector in order to extract these CP-odd observables. We discuss the role of zero modes in the CP-odd Green's function and show that, in the quenched approximation, there is a power divergence in the quark mass for CP-odd quantities at finite volume.Comment: 12 pages, revised manuscript to be publishe
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