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  2. notes.dvi

    www.statslab.cam.ac.uk/~grg/papers/USstflour.pdf
    15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMS. Georey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation
  3. notes.dvi

    www.statslab.cam.ac.uk/~grg/papers/USrednotes.pdf
    15 Aug 2012: PERCOLATION ANDDISORDERED SYSTEMSGeorey GRIMMETT. 2PREFACEThis course aims to be a (nearly) self-contained account of part of the mathematicaltheory of percolation and related topics. The rst nine chapters summarise rigorousresults in percolation
  4. rctree.dvi

    www.statslab.cam.ac.uk/~grg/papers/USrctree.pdf
    15 Aug 2012: BRANCHING PROCESSES, AND. RANDOM-CLUSTER MEASURES ON TREES. Geoffrey Grimmett, Svante JansonAbstra t. Random-cluster measures on infinite regular trees are studied in con-junction with a general type of ‘boundary condition’, namely an
  5. rcproc.dvi

    www.statslab.cam.ac.uk/~grg/papers/USrcproc.pdf
    15 Aug 2012: φbp,q = αφ′ (1 α)φ′′. for some distinct φ′,φ′′ Rp,q. It follows by [24, Thm. ... The given statement for θ0 may be proved similarly, making use of Theorem3.2 and [24, Prop.
  6. potts2.dvi

    www.statslab.cam.ac.uk/~grg/papers/USpotts2.pdf
    15 Aug 2012: POTTS MODELS AND RANDOM-CLUSTER. PROCESSES WITH MANY-BODY INTERACTIONS. Geoffrey GrimmettAbstra t. Known differential inequalities for certain ferromagnetic Potts models with pair-interactions may be extended to Potts models with many-body
  7. pinball.dvi

    www.statslab.cam.ac.uk/~grg/papers/USpinball.pdf
    15 Aug 2012: Rotator pin-ball. Ruijgrok and Cohen [24] have proposed a general studyof mirror and rotator' models. ... Quas, A., Some properties of Lorentz lattice gas models (1996) (to appear).24.
  8. opt.dvi

    www.statslab.cam.ac.uk/~grg/papers/USopt.pdf
    15 Aug 2012: See [24, 51, 52] for more informa-tion and references.Few non-trivial facts are known about the limit set L, and much eort hasbeen spent, largely inconclusively, on attempting to
  9. meanf.dvi

    www.statslab.cam.ac.uk/~grg/papers/USmeanf.pdf
    15 Aug 2012: THE RANDOM-CLUSTER MODEL. ON THE COMPLETE GRAPH. Béla Bollobás, Geoffrey Grimmett, Svante JansonAbstract. The random-cluster model of Fortuin and Kasteleyn contains as specialcases the percolation, Ising, and Potts models of statistical physics.
  10. mcst.dvi

    www.statslab.cam.ac.uk/~grg/papers/USmcst.pdf
    15 Aug 2012: 24 C. BEZUIDENHOUT, G. GRIMMETT, A. LOFFLERwhence, by Wald's equation ([13], p.
  11. keane.dvi

    www.statslab.cam.ac.uk/~grg/papers/USkeane.pdf
    15 Aug 2012: Theorem 6. [24] We have that µp(K = 1) = 1 whenever p > pentc. ... Soc., 130:175–188, 2001. MR1797779. [24] O. Häggström. Uniqueness of the infinite entangled component in three-dimensional bond percolation.

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