81,908 research outputs found

    On Uniqueness And Existence of Conformally Compact Einstein Metrics with Homogeneous Conformal Infinity

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    In this paper we show that for a generalized Berger metric g^\hat{g} on S3S^3 close to the round metric, the conformally compact Einstein (CCE) manifold (M,g)(M, g) with (S3,[g^])(S^3, [\hat{g}]) as its conformal infinity is unique up to isometries. For the high-dimensional case, we show that if g^\hat{g} is an SU(k+1)\text{SU}(k+1)-invariant metric on S2k+1S^{2k+1} for k1k\geq1, the non-positively curved CCE metric on the (2k+1)(2k+1)-ball B1(0)B_1(0) with (S2k+1,[g^])(S^{2k+1}, [\hat{g}]) as its conformal infinity is unique up to isometries. In particular, since in \cite{LiQingShi}, we proved that if the Yamabe constant of the conformal infinity Y(S2k+1,[g^])Y(S^{2k+1}, [\hat{g}]) is close to that of the round sphere then any CCE manifold filled in must be negatively curved and simply connected, therefore if g^\hat{g} is an SU(k+1)\text{SU}(k+1)-invariant metric on S2k+1S^{2k+1} which is close to the round metric, the CCE metric filled in is unique up to isometries. Using the continuity method, we prove an existence result of the non-positively curved CCE metric with prescribed conformal infinity (S2k+1,[g^])(S^{2k+1}, [\hat{g}]) when the metric g^\hat{g} is SU(k+1)\text{SU}(k+1)-invariant.Comment: Comments are welcome

    Measuring the ratio of HWWHWW and HZZHZZ couplings through W+WHW^+W^-H production

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    For a generic Higgs boson, measuring the relative sign and magnitude of its couplings with the WW and ZZ bosons is essential in determining its origin. Such a test is also indispensable for the 125-GeV Higgs boson. We propose that the ratio of the HWWHWW and HZZHZZ couplings λWZ\lambda_{WZ} can be directly determined through the W+WHW^+W^-H production, where HH denotes a generic Higgs boson, owing to the tree-level interference effect. While this is impractical at the LHC due to the limited sensitivity, it can be done at future e+ee^+e^- colliders, such as a 500-GeV ILC with the beam polarization P(e,e+)=(0.8,+0.3)P(e^-,e^+)=(-0.8,+0.3) in the jj±bbjj\ell^{\pm}bb and ±±jj\ell^{\pm}\ell^{\pm}\ell^{\mp}jj channels. The discovery potential of a general ratio and the power to discriminate it from the SM value are studied in detail. Combining the cross section of e+eW+WHe^+e^-\to W^+ W^- H with the measurements of HZZHZZ coupling at the HL-LHC, one can further improve the sensitivity of λWZ\lambda_{WZ}.Comment: 24 pages, 10 figures, 2 table

    Virtual moduli cycles and Gromov-Witten invariants of algebraic varieties

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    We introduce a method of constructing the virtual cycle of any scheme associated with a tangent-obstruction complex. We apply this method to constructing the virtual moduli cycle of the moduli of stable maps from n-pointed genus g curves to any smooth projective variety. As an application, we give an algebraic definition of GW-invariants for any smooth projective variety.Comment: 68 pages, Amstex. Revised version. It appeared in J. of Amer. Math. Soc. Jan 9
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