2,942 research outputs found

    Mining whole sample mass spectrometry proteomics data for biomarkers: an overview

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    In this paper we aim to provide a concise overview of designing and conducting an MS proteomics experiment in such a way as to allow statistical analysis that may lead to the discovery of novel biomarkers. We provide a summary of the various stages that make up such an experiment, highlighting the need for experimental goals to be decided upon in advance. We discuss issues in experimental design at the sample collection stage, and good practise for standardising protocols within the proteomics laboratory. We then describe approaches to the data mining stage of the experiment, including the processing steps that transform a raw mass spectrum into a useable form. We propose a permutation-based procedure for determining the significance of reported error rates. Finally, because of its general advantages in speed and cost, we suggest that MS proteomics may be a good candidate for an early primary screening approach to disease diagnosis, identifying areas of risk and making referrals for more specific tests without necessarily making a diagnosis in its own right. Our discussion is illustrated with examples drawn from experiments on bovine blood serum conducted in the Centre for Proteomic Research (CPR) at Southampton University

    Potts-Percolation-Gauss Model of a Solid

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    We study a statistical mechanics model of a solid. Neighboring atoms are connected by Hookian springs. If the energy is larger than a threshold the "spring" is more likely to fail, while if the energy is lower than the threshold the spring is more likely to be alive. The phase diagram and thermodynamic quantities, such as free energy, numbers of bonds and clusters, and their fluctuations, are determined using renormalization-group and Monte-Carlo techniques.Comment: 10 pages, 12 figure

    Ground State Entropy of the Potts Antiferromagnet on Cyclic Strip Graphs

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    We present exact calculations of the zero-temperature partition function (chromatic polynomial) and the (exponent of the) ground-state entropy S0S_0 for the qq-state Potts antiferromagnet on families of cyclic and twisted cyclic (M\"obius) strip graphs composed of pp-sided polygons. Our results suggest a general rule concerning the maximal region in the complex qq plane to which one can analytically continue from the physical interval where S0>0S_0 > 0. The chromatic zeros and their accumulation set B{\cal B} exhibit the rather unusual property of including support for Re(q)<0Re(q) < 0 and provide further evidence for a relevant conjecture.Comment: 7 pages, Latex, 4 figs., J. Phys. A Lett., in pres

    Mean Field Renormalization Group for the Boundary Magnetization of Strip Clusters

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    We analyze in some detail a recently proposed transfer matrix mean field approximation which yields the exact critical point for several two dimensional nearest neighbor Ising models. For the square lattice model we show explicitly that this approximation yields not only the exact critical point, but also the exact boundary magnetization of a semi--infinite Ising model, independent of the size of the strips used. Then we develop a new mean field renormalization group strategy based on this approximation and make connections with finite size scaling. Applying our strategy to the quadratic Ising and three--state Potts models we obtain results for the critical exponents which are in excellent agreement with the exact ones. In this way we also clarify some advantages and limitations of the mean field renormalization group approach.Comment: 16 pages (plain TeX) + 8 figures (PostScript, appended), POLFIS-TH.XX/9

    Ground State Entropy of Potts Antiferromagnets on Cyclic Polygon Chain Graphs

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    We present exact calculations of chromatic polynomials for families of cyclic graphs consisting of linked polygons, where the polygons may be adjacent or separated by a given number of bonds. From these we calculate the (exponential of the) ground state entropy, WW, for the q-state Potts model on these graphs in the limit of infinitely many vertices. A number of properties are proved concerning the continuous locus, B{\cal B}, of nonanalyticities in WW. Our results provide further evidence for a general rule concerning the maximal region in the complex q plane to which one can analytically continue from the physical interval where S0>0S_0 > 0.Comment: 27 pages, Latex, 17 figs. J. Phys. A, in pres

    Exact sampling from non-attractive distributions using summary states

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    Propp and Wilson's method of coupling from the past allows one to efficiently generate exact samples from attractive statistical distributions (e.g., the ferromagnetic Ising model). This method may be generalized to non-attractive distributions by the use of summary states, as first described by Huber. Using this method, we present exact samples from a frustrated antiferromagnetic triangular Ising model and the antiferromagnetic q=3 Potts model. We discuss the advantages and limitations of the method of summary states for practical sampling, paying particular attention to the slowing down of the algorithm at low temperature. In particular, we show that such a slowing down can occur in the absence of a physical phase transition.Comment: 5 pages, 6 EPS figures, REVTeX; additional information at http://wol.ra.phy.cam.ac.uk/mackay/exac

    Families of Graphs with W_r({G},q) Functions That Are Nonanalytic at 1/q=0

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    Denoting P(G,q)P(G,q) as the chromatic polynomial for coloring an nn-vertex graph GG with qq colors, and considering the limiting function W({G},q)=limnP(G,q)1/nW(\{G\},q) = \lim_{n \to \infty}P(G,q)^{1/n}, a fundamental question in graph theory is the following: is Wr({G},q)=q1W({G},q)W_r(\{G\},q) = q^{-1}W(\{G\},q) analytic or not at the origin of the 1/q1/q plane? (where the complex generalization of qq is assumed). This question is also relevant in statistical mechanics because W({G},q)=exp(S0/kB)W(\{G\},q)=\exp(S_0/k_B), where S0S_0 is the ground state entropy of the qq-state Potts antiferromagnet on the lattice graph {G}\{G\}, and the analyticity of Wr({G},q)W_r(\{G\},q) at 1/q=01/q=0 is necessary for the large-qq series expansions of Wr({G},q)W_r(\{G\},q). Although WrW_r is analytic at 1/q=01/q=0 for many {G}\{G\}, there are some {G}\{G\} for which it is not; for these, WrW_r has no large-qq series expansion. It is important to understand the reason for this nonanalyticity. Here we give a general condition that determines whether or not a particular Wr({G},q)W_r(\{G\},q) is analytic at 1/q=01/q=0 and explains the nonanalyticity where it occurs. We also construct infinite families of graphs with WrW_r functions that are non-analytic at 1/q=01/q=0 and investigate the properties of these functions. Our results are consistent with the conjecture that a sufficient condition for Wr({G},q)W_r(\{G\},q) to be analytic at 1/q=01/q=0 is that {G}\{G\} is a regular lattice graph Λ\Lambda. (This is known not to be a necessary condition).Comment: 22 pages, Revtex, 4 encapsulated postscript figures, to appear in Phys. Rev.
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