8,262 research outputs found

    Microwave interferometry of Saturn: Application to the brightness temperature of the rings

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    Radio interferometric measurements of Saturn and Saturn's rings are explained. The measurements are limited to Mu is greater than or equal to 3. Data are also given on visibility functions, flux density, and brightness temperature

    Lepton-mass effects in the decays HZZ+τ+τH \to ZZ^{\ast} \to \ell^{+} \ell^{-} \tau^{+} \tau^{-} and HWWντντH \to WW^{\ast} \to \ell \nu \tau \nu_{\tau}

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    We consider lepton-mass effects in the cascade decays HZ(+)+Z(τ+τ)H\to Z(\to \ell^{+} \ell^{-})+Z^{\ast}(\to \tau^{+}\tau^{-}) and HW(νˉ)+W+(τ+ντ)H\to W^{-}(\to \ell^{-}\bar \nu_{\ell})+W^{+\ast}(\to \tau^{+}\nu_{\tau}). Since the scale of the problem is set by the off-shellness q2q^{2} of the respective gauge bosons in the limits (m+m)2q2(mHmW,Z)2(m_{\ell}+m_{\ell'})^{2} \le q^{2} \le (m_{H}-m_{W,Z})^{2} and not by mW,Z2m_{W,Z}^{2}, lepton-mass effects are non-negligible for the τ\tau modes in particular close to the threshold of the off-shell decays. Lepton-mass effects show up e.g.\ in the three-fold joint angular decay distribution for the decays. Nonzero lepton masses lead to leptonic helicity-flip contributions which in turn can generate novel angular dependencies in the respective three-fold angular decay distributions. Lepton-mass effects are more pronounced in the HZ()Z(ττ)H \to Z(\to \ell\ell)Z^{\ast}(\to\tau\tau) mode which, in part, is due to the fact that the ratio of lepton helicity flip/nonflip contributions in the decay Z+Z^{\ast} \to \ell^{+}\ell^{-} is four times larger than in the decay W++νW^{+\ast}\to \ell^{+}\nu. We also briefly consider the corresponding off-shell -- off-shell decays HZ(+)+Z(τ+τ)H\to Z^{\ast}(\to \ell^{+}\ell^{-})+Z^{\ast}(\to \tau^{+}\tau^{-}) and HW(νˉ)+W+(τ+ντ)H\to W^{-\ast}(\to \ell^{-}\bar \nu_{\ell})+W^{+\ast}(\to \tau^{+}\nu_{\tau}).Comment: 45 pages, 9 figures and 6 tables, published versio

    Neutrino-Nucleus Cross Section Measurements using Stopped Pions and Low Energy Beta Beams

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    Two new facilities have recently been proposed to measure low energy neutrino-nucleus cross sections, the nu-SNS (Spallation Neutron Source) and low energy beta beams. The former produces neutrinos by pion decay at rest, while the latter produces neutrinos from the beta decays of accelerated ions. One of the uses of neutrino-nucleus cross section measurements is for supernova studies, where typical neutrino energies are 10s of MeV. In this energy range there are many different components to the nuclear response and this makes the theoretical interpretation of the results of such an experiment complex. Although even one measurement on a heavy nucleus such as lead is much anticipated, more than one data set would be still better. We suggest that this can be done by breaking the electron spectrum down into the parts produced in coincidence with one or two neutrons, running a beta beam at more than one energy, comparing the spectra produced with pions and a beta beam or any combination of these.Comment: 6 pages, 6 figure

    Conflict-Free Coloring Made Stronger

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    In FOCS 2002, Even et al. showed that any set of nn discs in the plane can be Conflict-Free colored with a total of at most O(logn)O(\log n) colors. That is, it can be colored with O(logn)O(\log n) colors such that for any (covered) point pp there is some disc whose color is distinct from all other colors of discs containing pp. They also showed that this bound is asymptotically tight. In this paper we prove the following stronger results: \begin{enumerate} \item [(i)] Any set of nn discs in the plane can be colored with a total of at most O(klogn)O(k \log n) colors such that (a) for any point pp that is covered by at least kk discs, there are at least kk distinct discs each of which is colored by a color distinct from all other discs containing pp and (b) for any point pp covered by at most kk discs, all discs covering pp are colored distinctively. We call such a coloring a {\em kk-Strong Conflict-Free} coloring. We extend this result to pseudo-discs and arbitrary regions with linear union-complexity. \item [(ii)] More generally, for families of nn simple closed Jordan regions with union-complexity bounded by O(n1+α)O(n^{1+\alpha}), we prove that there exists a kk-Strong Conflict-Free coloring with at most O(knα)O(k n^\alpha) colors. \item [(iii)] We prove that any set of nn axis-parallel rectangles can be kk-Strong Conflict-Free colored with at most O(klog2n)O(k \log^2 n) colors. \item [(iv)] We provide a general framework for kk-Strong Conflict-Free coloring arbitrary hypergraphs. This framework relates the notion of kk-Strong Conflict-Free coloring and the recently studied notion of kk-colorful coloring. \end{enumerate} All of our proofs are constructive. That is, there exist polynomial time algorithms for computing such colorings
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