49,467 research outputs found

    On Chow Stability for algebraic curves

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    In the last decades there have been introduced different concepts of stability for projective varieties. In this paper we give a natural and intrinsic criterion of the Chow, and Hilbert, stability for complex irreducible smooth projective curves CPnC\subset \mathbb P ^n. Namely, if the restriction TPCnT\mathbb P_{|C} ^n of the tangent bundle of Pn\mathbb P ^n to CC is stable then CPnC\subset \mathbb P ^n is Chow stable, and hence Hilbert stable. We apply this criterion to describe a smooth open set of the irreducible component HilbChP(t),sHilb^{P(t),s}_{{Ch}} of the Hilbert scheme of Pn\mathbb{P} ^n containing the generic smooth Chow-stable curve of genus gg and degree d>g+ngn+1.d>g+n-\left\lfloor\frac{g}{n+1}\right\rfloor. Moreover, we describe the quotient stack of such curves. Similar results are obtained for the locus of Hilbert stable curves.Comment: Minor corrections and improvements to presentation. We add Theorem 4.

    A Layman's guide to SUSY GUTs

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    The determination of the most straightforward evidence for the existence of the Superworld requires a guide for non-experts (especially experimental physicists) for them to make their own judgement on the value of such predictions. For this purpose we review the most basic results of Super-Grand unification in a simple and clear way. We focus the attention on two specific models and their predictions. These two models represent an example of a direct comparison between a traditional unified-theory and a string-inspired approach to the solution of the many open problems of the Standard Model. We emphasize that viable models must satisfy {\em all} available experimental constraints and be as simple as theoretically possible. The two well defined supergravity models, SU(5)SU(5) and SU(5)×U(1)SU(5)\times U(1), can be described in terms of only a few parameters (five and three respectively) instead of the more than twenty needed in the MSSM model, \ie, the Minimal Supersymmetric extension of the Standard Model. A case of special interest is the strict no-scale SU(5)×U(1)SU(5)\times U(1) supergravity where all predictions depend on only one parameter (plus the top-quark mass). A general consequence of these analyses is that supersymmetric particles can be at the verge of discovery, lurking around the corner at present and near future facilities. This review should help anyone distinguish between well motivated predictions and predictions based on arbitrary choices of parameters in undefined models.Comment: 25 pages, Latex, 11 figures (not included), CERN-TH.7077/93, CTP-TAMU-65/93. A complete ps file (1.31MB) with embedded figures is available by request from [email protected]

    Radion Assisted Gauge Inflation

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    We propose an extension to the recently proposed extranatural or gauge inflation scenario in which the radius modulus field around which the Wilson loop is wrapped assists inflation as it shrinks. We discuss how this might lead to more generic initial conditions for inflation.Comment: 10 pages, 2 figure

    SUSY signals at HERA in the no-scale flipped SU(5) supergravity model

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    Sparticle production and detection at HERA are studied within the recently proposed no-scale flipped SU(5)SU(5) supergravity model. Among the various reaction channels that could lead to sparticle production at HERA, only the following are within its limit of sensitivity in this model: epe~L,Rχi0+X,ν~eχ1+Xe^-p\to \tilde e^-_{L,R}\chi^0_i+X, \tilde \nu_e\chi^-_1+X, where χi0(i=1,2)\chi^0_i(i=1,2) are the two lightest neutralinos and χ1\chi^-_1 is the lightest chargino. We study the elastic and deep-inelastic contributions to the cross sections using the Weizs\"acker-Williams approximation. We find that the most promising supersymmetric production channel is right-handed selectron (e~R\tilde e_{R}) plus first neutralino (χ10\chi^0_1), with one hard electron and missing energy signature. The ν~eχ1\tilde\nu_e\chi^-_1 channel leads to comparable rates but also allows jet final states. A right-handedly polarized electron beam at HERA would shut off the latter channel and allow preferentially the former one. With an integrated luminosity of {\cal L}=100\ipb, HERA can extend the present LEPI lower bounds on me~R,mν~e,mχ10m_{\tilde e_R}, m_{\tilde\nu_e},m_{\chi^0_1} by \approx25\GeV, while {\cal L}=1000\ipb will make HERA competitive with LEPII. We also show that the Leading Proton Spectrometer (LPS) at HERA is an excellent supersymmetry detector which can provide indirect information about the sparticle masses by measuring the leading proton longitudinal momentum distribution.Comment: 11 pages, 8 figures (available upon request as uuencoded file or separate ps files), tex (harvmac) CTP-TAMU-15/93, CERN/LAA/93-1

    Supersymmetry dileptons and trileptons at the Tevatron

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    We consider the production of supersymmetry neutralinos and charginos in ppˉp\bar p collisions at the Tevatron, and their subsequent decay via hadronically quiet dileptons and trileptons. We perform our computations in the context of a variety of supergravity models, including generic four-parameter supergravity models, the minimal SU(5)SU(5) supergravity model, and SU(5)×U(1)SU(5)\times U(1) supergravity with string inspired two- and one-parameter moduli and dilaton scenarios. Our results are contrasted with estimated experimental sensitivities for dileptons and trileptons for integrated luminosities of 100\ipb and 1\ifb, which should be available in the short and long terms. We find that the dilepton mode is a needed complement to the trilepton signal when the latter is suppressed by small neutralino leptonic branching ratios. The estimated reaches in chargino masses can be as large as 100\,(150)\GeV for 100\ipb\,(1\ifb). We also discuss the task left for LEPII once the Tevatron has completed its short-term search for dilepton and trilepton production.Comment: 12 pages (LaTeX), 6 figures (included

    SPAN: Astronomy and astrophysics

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    The Space Physics Analysis Network (SPAN) is a multi-mission, correlative data comparison network which links science research and data analysis computers in the U.S., Canada, and Europe. The purpose of this document is to provide Astronomy and Astrophysics scientists, currently reachable on SPAN, with basic information and contacts for access to correlative data bases, star catalogs, and other astrophysic facilities accessible over SPAN

    Disk stars in the Milky Way detected beyond 25 kpc from its center

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    CONTEXT. The maximum size of the Galactic stellar disk is not yet known. Some studies have suggested an abrupt drop-off of the stellar density of the disk at Galactocentric distances R15R\gtrsim 15 kpc, which means that in practice no disk stars or only very few of them should be found beyond this limit. However, stars in the Milky Way plane are detected at larger distances. In addition to the halo component, star counts have placed the end of the disk beyond 20 kpc, although this has not been spectroscopically confirmed so far. AIMS. Here, we aim to spectroscopically confirm the presence of the disk stars up to much larger distances. METHODS. With data from the LAMOST and SDSS-APOGEE spectroscopic surveys, we statistically derived the maximum distance at which the metallicity distribution of stars in the Galactic plane is distinct from that of the halo populations. RESULTS. Our analysis reveals the presence of disk stars at R>26 kpc (99.7% C.L.) and even at R>31 kpc (95.4% C.L.).Comment: 4 pages, accepted to be published in A&A-Letter

    Experimental aspects of SU(5)xU(1) supergravity

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    We study various aspects of SU(5)×U(1)SU(5)\times U(1) supergravity as they relate to the experimental verification or falsification of this model. We consider two string-inspired, universal, one-parameter, no-scale soft-supersymmetry-breaking scenarios, driven by the FF-terms of the moduli and dilaton fields. The model is described in terms of the supersymmetry mass scale (\ie, the chargino mass mχ1±m_{\chi^\pm_1}), tanβ\tan\beta, and the top-quark mass. We first determine the combined effect on the parameter space of all presently available direct and indirect experimental constraints, including the LEP lower bounds on sparticle and Higgs-boson masses, the bsγb\to s\gamma rate, the anomalous magnetic moment of the muon, the high-precision electroweak parameters ϵ1,ϵb\epsilon_1,\epsilon_b (which imply m_t\lsim180\GeV), and the muon fluxes in underground detectors (neutrino telescopes). For the still-allowed points in (mχ1±,tanβ)(m_{\chi^\pm_1},\tan\beta) parameter space, we re-evaluate the experimental situation at the Tevatron, LEPII, and HERA. In the 1994 run, the Tevatron could probe chargino masses as high as 100 GeV. At LEPII the parameter space could be explored with probes of different resolutions: Higgs boson searches, selectron searches, and chargino searches. Moreover, for m_t\lsim150\GeV, these Higgs-boson searches could explore all of the allowed parameter space with \sqrt{s}\lsim210\GeV.Comment: latex, 36 pages, 25 figures (not included). Figures are available via anonymous ftp from hplaa02.cern.ch (/pub/lopez) as either 33 ps files (Easpects*.ps, 8.1MB) or one uuencoded file (AllFigures.uu, 3.7MB
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