1,017 research outputs found

    Improved Currents for Heavy Quarks

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    We discuss lattice artifacts for matrix elements of hadrons containing one or more heavy quark. In particular, we analyze interrelations between lattice artifacts and the 1/mQ1/m_Q expansion. The implications for calculations of heavy-light decay constants and of semi-leptonic form factors are discussed.Comment: 3 pages, no figures, uuencoded PostScript, proceedings of Lattice '94. LaTeX at ftp://fnth06.fnal.gov/pub/Fermilab-Pub/95.00

    The Charm Quark on the Lattice

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    We formulate lattice fermions in a way that encompasses Wilson fermions as well as the static and non-relativistic approximations. In particular, we treat mqam_qa systematically (mqm_q is the fermion mass) showing how to understand the Wilson action as an effective action for systems with \vek{p}\ll m_q. The results show how to extract matrix elements and the spectrum from simulations with mqa≈1m_qa\approx1, which is relevant for the charm quark.Comment: 4 pages LaTeX using espcrc2.sty and epsf.sty. FERMILAB-CONF-92/329-

    Binding Energies in Nonrelativistic Field Theories

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    Relativistic corrections communicate the binding energy of a bound state to its kinetic mass. This mechanism is reviewed and used to explain anomalous results of Collins, Edwards, Heller, and Sloan (hep-lat/9512026), which compared rest and kinetic masses of heavy-light mesons and quarkonia.Comment: 4 pages, 1 figure, poster presented at LATTICE96(heavy quarks

    Trees whose 2-domination subdivision number is 2

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    A set SS of vertices in a graph G=(V,E)G = (V,E) is a 22-dominating set if every vertex of V∖SV\setminus S is adjacent to at least two vertices of SS. The 22-domination number of a graph GG, denoted by γ2(G)\gamma_2(G), is the minimum size of a 22-dominating set of GG. The 22-domination subdivision number sdγ2(G)sd_{\gamma_2}(G) is the minimum number of edges that must be subdivided (each edge in GG can be subdivided at most once) in order to increase the 22-domination number. The authors have recently proved that for any tree TT of order at least 33, 1≤sdγ2(T)≤21 \leq sd_{\gamma_2}(T)\leq 2. In this paper we provide a constructive characterization of the trees whose 22-domination subdivision number is 22

    The Signed Roman Domatic Number of a Digraph

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    Let DD be a finite and simple digraph with vertex set V(D)V(D).A {\em signed Roman dominating function} on the digraph DD isa function f:V(D)⟶{−1,1,2}f:V (D)\longrightarrow \{-1, 1, 2\} such that∑u∈N−[v]f(u)≥1\sum_{u\in N^-[v]}f(u)\ge 1 for every v∈V(D)v\in V(D), where N−[v]N^-[v] consists of vv andall inner neighbors of vv, and every vertex u∈V(D)u\in V(D) for which f(u)=−1f(u)=-1 has an innerneighbor vv for which f(v)=2f(v)=2. A set {f1,f2,…,fd}\{f_1,f_2,\ldots,f_d\} of distinct signedRoman dominating functions on DD with the property that ∑i=1dfi(v)≤1\sum_{i=1}^df_i(v)\le 1 for eachv∈V(D)v\in V(D), is called a {\em signed Roman dominating family} (of functions) on DD. The maximumnumber of functions in a signed Roman dominating family on DD is the {\em signed Roman domaticnumber} of DD, denoted by dsR(D)d_{sR}(D). In this paper we initiate the study of signed Romandomatic number in digraphs and we present some sharp bounds for dsR(D)d_{sR}(D). In addition, wedetermine the signed Roman domatic number of some digraphs. Some of our results are extensionsof well-known properties of the signed Roman domatic number of graphs

    Fouling Characteristics of a Light Australian Crude Oil

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    Australian crude oils, which generally contain little asphaltenes, nevertheless give rise to fouling in refinery pre-heat trains. In this research, fouling of a series of such crude oils and their blends is being assessed. The present work focuses on thermal fouling resulting from heating Gippsland crude oil at moderate temperatures. The oil is maintained under nitrogen at a pressure of 379 kPa, and re-circulated at bulk temperatures of 80-120°C through an electrically heated annular probe at velocities in the range 0.25 to 0.65 m/s with surface temperatures from 180-260°C. Experiments are run for periods up to 90 hours at constant heat flux. Fouling is detected by the increase of wall temperature of the probe. The oil is characterized by its filterable solids content, density and viscosity both before and after the fouling run. The trends in fouling rates are compared to predictions of the threshold-fouling model proposed by Ebert and Panchal (1995). Data on deposit composition are presented, and the fouling mechanism discussed
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