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  2. Boundary Conditions at Walls for CMC

    www3.eng.cam.ac.uk/~em257/LectNotes_all.pdf
    3 Feb 2013: 2 (pp. 6-20) for the. atmospheric structure. For those who like chemistry and who want to follow Air Quality. ... 5R18: Environmental Fluid Mechanics Pollution dispersion in the environment. 20. Example 2.3.
  3. Dr Nicholas Hine I am a Winton Advanced Research ...

    www.tcm.phy.cam.ac.uk/~ndmh3/cv.pdf
    21 Feb 2013: Chem. Phys. 133, 114111 (2010). [20] D.D. O'Regan, N.D.M. Hine, A.A.
  4. Annex: Sample exam questions, 2011 and 1980s Sample questions ...

    www.tcm.phy.cam.ac.uk/~mw141/Annex-current-1980s-Qs-small.pdf
    20 Apr 2013: 1.16 107 kg of air, travelling at a speed of 20 m s–1, pass through the turbine each. ... Discussion of principles required, since next part only [2]. calculation. Insertion of numbers only 3/20.
  5. Adiabatic Continuation of Fractional Chern Insulators to Fractional…

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.109.246805.pdf
    14 Jan 2013: 20]. There are several proposals forconstructing FCI wave functions [21–27], and some overlapswere calculated for fermionic systems [26]. ... The periodicLandau-level orbitals jðx; yÞ, j 0;. ; N 1 [42,43]are chosen with definite momenta ky 2j=L2,
  6. PHYSICAL REVIEW B 86, 165314 (2012) Particle entanglement spectra ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.86.165314.pdf
    14 Jan 2013: 2 4 6 8. 10 12 14 16 18 20. 0 2 4 6 8 10. ... 0. 5. 10. 15. 20. 25. -1 0 1 2 3 4 5 6.
  7. Lecture I 1 Lecture I: Collective Excitations: From Particles ...

    www.tcm.phy.cam.ac.uk/~bds10/tp3/lectures.pdf
    10 Nov 2013: ka†k. )] O(N. 1/20 ). cf. quantum AF in spin-wave approximation. ... N.B. Momentum conservation eliminates terms at O(N3/20 ). Physical interpretation of components:.
  8. MR-excitations_Koeln_May-12

    www.tcm.phy.cam.ac.uk/BIG/gm360/MR-excitations_Koeln_web.pdf
    30 Jul 2013: a) N=12, 2l=22 (b) N=12, 2l=20. w=0. w=3λ. L=02. 3 0. ... 0. blue: Nφ=20 (σ=4). (a) N=12, ν=5/2, w=3λ. E-E. sky. (e2/λ. ).
  9. Lattice_PES_Dresden

    www.tcm.phy.cam.ac.uk/BIG/gm360/Lattice_PES_Dresden_Web.pdf
    30 Jul 2013: 4. 6. 8. 10. 12. 14. 16. 18. 20. 0 2 4 6 8 10. ... 10. 12. 14. 16. 18. 20. 0 2 4 6 8 10.
  10. Dynamics and Thermodynamics of Artificial Spin Ices - and the Role of …

    www.tcm.phy.cam.ac.uk/BIG/gm360/ArtIcePhoenix2011.pdf
    30 Jul 2013: 0. 20. 40. 60. 80. %. Type I Type II Type III Type IV. ... 30. -20. -10. 0. 10. 20. 30. %. Type IType IIType IIIType IV.
  11. Tutorial Bandit Processes and Index Policies Richard Weber,…

    www.statslab.cam.ac.uk/~rrw1/talks/YETQweber2013.pdf
    14 Nov 2013: 20 / 52. Some constraints. Let xπi = Eπ(Ni)/µi be the mean work-in-system of class i. ... 20 / 52. A mathematical program. Consider the optimization problem. minimizeπ.
  12. A More General Pandora’s Rule Richard Weber, University of ...

    www.statslab.cam.ac.uk/~rrw1/talks/LSEseminar13113.pdf
    14 Nov 2013: Is a generalization of Pandora rule evaporating? 20/57 ,. Yet even more necessity! ... Is a generalization of Pandora rule evaporating? 20/57 ,. Sufficiency. Theorem 1 Suppose u has the form described as necessary, i.e.
  13. Statistics

    www.statslab.cam.ac.uk/~rrw1/stats/index.html
    31 Jul 2013: One in 750,000? One in 20,000? One in 15,000,000? Wikipedai entriies of some famous statisticians: Bayes (Bayesian inference), Gosset (Student's t-distribution), Neyman (Neyman-Pearson test),
  14. Richard Weber's Publications

    www.statslab.cam.ac.uk/~rrw1/publications/papers.html
    8 Nov 2013: C. Courcoubetis and R. R. Weber, Economic issues in shared infrastructures, IEEE/ACM Transactions on Networking, 20: 594-608, 2012.
  15. 22 May 2013: 19. 5.5 Example: optimal parking. 20. i. 6 Optimal Stopping Problems 21. ... 20. 6 Optimal Stopping Problems. More on stopping problems and their solution.
  16. 22 May 2013: 20. 6 Random walks in dimensions one, two and three. 6.1 Simple random walk on Z.
  17. Discussion of Large Covariance Estimation by Thresholding Principal…

    www.statslab.cam.ac.uk/~rjs57/YuSamworthDisc.pdf
    3 Sep 2013: Econo-metrica, 70, 191–221. 2. 800000. 1200000. 1600000. 5 10 15 20. ... 1500. 1600. 1700. (c). 8.0e07. 1.2e08. 1.6e08. 5 10 15 20.
  18. WIAS2013.dvi

    www.statslab.cam.ac.uk/~rjs57/WIAS2013.pdf
    3 Feb 2013: E|f̃n(x0) f(x0)|. c(d){ det(2φ0(x0)). f(x0)2. }1/(d4). February 3, 2013- 20. R. ... 0.00. 0.10. 0.20. 0.30. s. Mar. gina. l Den. sitie. s.
  19. Uniformity of the late points of random walk on Znd for d 3

    www.statslab.cam.ac.uk/~ps422/rwunif2.pdf
    12 Sep 2013: nψ exp(cδ2nβ(d2)ψ. ) ecn. ψ. (2.20). For the second probability on the right side of (2.18), we apply Lemma 2.4 to obtain for allδ (0, ... 1 pd)rd2. (1 O. ( rR. ) O. (1. r2. )). (3.2). 20 JASON MILLER AND PERLA SOUSI. Proof. By Bayes’ formula we
  20. 10 Oct 2013: 20. 2.7 Uniformly integrable martingales. 21. 2.8 Backwards martingales. 23. 2.9 Applications of martingales. ... Xn‖p p. p 1‖Xn‖p,. 20. where recall that Xn = supkn |Xk|.
  21. Mixing times are hitting times of large sets Yuval ...

    www.statslab.cam.ac.uk/~ps422/mix-hit.pdf
    25 Apr 2013: Since tcts tL (see [6, Theorem 20.3]), Theorem 1.4gives a partial answer to that problem. ... V. Chacon. Stopping times for recurrent Markov processes. Illinois J.Math., 20(3):467–475, 1976.
  22. Nonparametric Bernstein-von Mises theorems in Gaussian white noise

    www.statslab.cam.ac.uk/~nickl/Site/__files/AOS1133.pdf
    28 Oct 2013: Consider a functional satisfying (20). Assume more-over either that is linear, or that for some sequence rn = o(n1/2),. ... θ0,lk /σl 1. (nσlu nσl θ0,lk. σl. )2ϕ(u) du. 2nσ 2l[θ 20,lk.
  23. QLE Jason Miller and Scott Sheffield MIT August 1, ...

    www.statslab.cam.ac.uk/~jpm205/slides/qleslides.pdf
    1 Aug 2013: Jason Miller and Scott Sheffield (MIT) QLE August 1, 2013 20 / 37.
  24. BOUNDS ON CONNECTIVE CONSTANTSOF REGULAR GRAPHS GEOFFREY R. GRIMMETT…

    www.statslab.cam.ac.uk/~grg/papers/saw2-final2.pdf
    26 Aug 2013: Part (a) may be found also in [20, Lemma 2.1], which appearedduring the writing of this paper. ... 20] H. Lacoin, Non-coincidence of quenched and annealed connective constants onthe supercritical planar percolation cluster, Probab.
  25. PERCOLATION OF FINITE CLUSTERSAND INFINITE SURFACES GEOFFREY R.…

    www.statslab.cam.ac.uk/~grg/papers/plaq-final.pdf
    7 Mar 2013: n. Then pFc < pSfin(F ). Proof of Theorem 1.1. When d 19 and S = F = 0, (4.3) is proved in[20]. ... 20] G. Kozma and A. Nachmias, Arm exponents in high dimensional percolation,J.
  26. Noname manuscript No.(will be inserted by the editor) Bond ...

    www.statslab.cam.ac.uk/~grg/papers/iso-final6.pdf
    21 May 2013: This is a continuation and extension of the work begun in [19,20]. ... substance. Therefore, further discussion is omitted, andthe reader is referred instead to [20, Sect.
  27. 11 Sep 2013: C1,kL(n)nγ1µnk 6 σn,k 6 C2,kL(n)n. γ1µnk, k = 1, 2. (20). ... We shall in fact use slightly less than this.Similarly to the proof of (17), by (19)–(20), there exists C1 < such that.
  28. Cluster detection in networks using percolation

    www.statslab.cam.ac.uk/~grg/papers/BEJ412.pdf
    14 Mar 2013: Remember thatσ 20 denotes the variance of F0. Cluster detection in networks using percolation 681. ... Let θ (β) = inft γθ |t (β)/σ 20|t , where, in congruence with Sections 5.1 and 5.2,.
  29. Universality for bond percolation in two dimensions

    www.statslab.cam.ac.uk/~grg/papers/AOP740.pdf
    12 Sep 2013: A different extension of the star–triangle method has been the subject of workdescribed in [2, 19, 20].
  30. 3 Jul 2013: Furthermore, work ofKesten [20] on scaling theory has provided the groundwork for exact calculationsof critical exponents for two-dimensional percolation (see [23, 29], e.g.).
  31. paper wear.dvi

    www.phase-trans.msm.cam.ac.uk/2013/Wear_Bakshi.pdf
    5 Nov 2013: 5. Wear 308 (2013) 46-53. in order to estimate the true thickness (t) using the relation [20]:. ... 29] W. C. Oliver, G. M. Pharr, J. Mater. Res. 19-1 (2004) 3–20.
  32. 28 May 2013: Lin, K.M. Lin, C.S. Lin, T.M. Ouyang, Corr. Sci. 44 (2002) 2013.[20] O. ... Temperature (K). 0. 200. 400. 600. 800. 1000. 1200. 0 20 40 60 80 100.
  33. surface.dvi

    www.phase-trans.msm.cam.ac.uk/2013/surface.pdf
    9 Oct 2013: 20] A. Juan, R. Hoffmann, Hydrogen on the fe (110) surface and near bulk bcc fevacancies: a comparative bonding study, Surface science, 421(1) (1999) 1–16. ... phase single H atom 0 layer 1 layer 3 layers. ferrite 0.19 0.24 0.20 0.19.
  34. LTT3

    www.phase-trans.msm.cam.ac.uk/2013/review_Ooi_MD_2014.pdf
    23 Dec 2013: residual stress in 3-dimensional detail without destroying the sample [8, 20, 21]. ... beyond the HAZ and that this is due to the unaccounted variant selection during simulation [20].
  35. Regeneration Technique for Welding Nanostructured Bainite

    www.phase-trans.msm.cam.ac.uk/2013/Regeneration.pdf
    3 May 2013: where bainite forms first [18-20]. As a result, the MS temperature is reduced to below. ... 0. $ 20. 0. $ 11. 1. Nanostructured bainite steel. Conventionally welded joint.
  36. Flash

    www.phase-trans.msm.cam.ac.uk/2013/Novelty_welding.pdf
    19 Feb 2013: Australasian Welding Journal, 55 (2011) 20--27. Australasian Welding Journal, 55 (2011) 20--27. ... Australasian Welding Journal, 55 (2011) 20--27.
  37. paper.dvi

    www.phase-trans.msm.cam.ac.uk/2013/Multiple.pdf
    20 Jun 2013: K. D. H. Bhadeshia: Mat. Sci. Techn. 20 (2004) 1499–1505. [9] D.
  38. Effect of retained austenite and high temperature Lavesphase on ...

    www.phase-trans.msm.cam.ac.uk/2013/maraging_Ooi_MSEA_2013.pdf
    4 Jan 2013: neering Materials, volume 345–346 I, pp. 189–192. [20] V. Seetharaman, R. ... 20. 8 (a) Effect of heating rate on the dilatation curve in the in-vestigated alloy.
  39. 02(2013-013).fm

    www.phase-trans.msm.cam.ac.uk/2013/macro.pdf
    14 Jun 2013: Many studies have sought to exper-imentally verify these models,20,21,48,167–169) but anothercommon approach has been to find functions by fittingexperimental results directly to Darcy’s
  40. Interphase precipitation in Ti–Nb and Ti–Nb–Mo bearing steel J. ...

    www.phase-trans.msm.cam.ac.uk/2013/interphase_Jang_MST_2013.pdf
    22 Feb 2013: elongation of some 20%. Typical compositions (wt-%) ofsuch steels are in the range12. ... Ingots 30 kg in weight were prepared by vacuuminduction melting and reheated to 1200uC for hot rollingto 20 mm thick plates with a finishing temperature.900uC.
  41. Program_monday_mitneu

    www.phase-trans.msm.cam.ac.uk/2013/ICAMS/program_icams2.pdf
    16 May 2013: 3:20-3:40 J. RogalAtomistic modelling of phase transformation kinetics. 3:40-4:10 Break Break. ... 3:20-3:50 Break Break. 3:50-4:30 D. RaabeNanoscale phase transformations at martensite interfaces.
  42. Computational Design of Advanced Steels H. K. D. H. ...

    www.phase-trans.msm.cam.ac.uk/2013/Genome.pdf
    27 Oct 2013: Thescale of the structure is known to decrease as the transformation temperatureis reduced [20]. ... H. Bhadeshia: Mat. Sci.Techn. 20 (2004) 814. [32] F. G. Caballero, M.
  43. IOP PUBLISHING SCIENCE AND TECHNOLOGY OF ADVANCED MATERIALS Sci. ...

    www.phase-trans.msm.cam.ac.uk/2013/first_Bhadeshia_STAM_2013.pdf
    16 Mar 2013: 3. Design. There are formidable difficulties in creating novelnanostructures which have the combination of propertiesappropriate for large-scale applications [20]. ... Sci. Technol. 20 814. [57] Caballero F G, Miller M K, Clarke A J and Garcia-Mateo
  44. Theory for Hydrogen Desorptionin Ferritic Steel Eun Ju Song ...

    www.phase-trans.msm.cam.ac.uk/2013/ferrite.pdf
    3 Jul 2013: hydrogen (i.e., during diffusion) and assuming no interactionsbetween the occupied sites, [20]:. ... ISIJInternational, 47:1131–1140, 2007. [20] R. A. Oriani. The diffusion and trapping of hydrogen in steel.
  45. paper.dvi

    www.phase-trans.msm.cam.ac.uk/2013/Cottrell_2013.pdf
    19 Oct 2013: D. H. Bhadeshia, A. R. Waugh, Acta Metallurgica 30 (1982) 775–784.[20] H. ... 20 (2004) 814–818.[27] F. G. Caballero, M. K. Miller, A. J.
  46. The Bainite Controversy Lucy Fielding M.Eng. Department of Materials…

    www.phase-trans.msm.cam.ac.uk/2013/controversy_Fielding_MST_2013.pdf
    4 Mar 2013: curves of pearlite and bainite [20]. This temperature is well below that at which pro-eutectoid ferrite. ... 20. Most exciting, however, was the use of hot-stage microscopy to observe the growth of individual subunits.
  47. hkdb.dvi

    www.phase-trans.msm.cam.ac.uk/2013/confocal.pdf
    11 Mar 2013: Wakasa and C. M. Wayman. Crystallography and morphology ofsurface martensite in Fe-20%Ni-5%Mn. ... 20] H. Kitahara, M. Ueda, N. Tsuji, and Y. Minamino. Variant selectionof plate martensite in Fe-28.5at.%Ni alloy.
  48. coarsening.dvi

    www.phase-trans.msm.cam.ac.uk/2013/coarsening_MST.pdf
    21 Jul 2013: A widely accepted theory for coarsening of a small fraction of precipitates,controlled by diffusion is given by the Lifshitz, Slyozov and Wagner (LSW)[18–20]:. ... Ardell, Acta Metallurgica 20 (1972) 61–71. [22] B. Sundman, B. Jansson, J.
  49. 12 May 2013: austenite grain size [20–22],and can readily be calculated. ... 20] H. S. Yang, H. K. D. H. Bhadeshia: Scripta Materialia 60 (2009) 493–495.[21] H.-S.
  50. anisotropy

    www.phase-trans.msm.cam.ac.uk/2013/anisotropy_Joo_ISIJ_2013.pdf
    19 Aug 2013: POSCO , 12:20–27, 2007. [6] K. Kim and J.-H. Bae. Metallurgical and process parameters for commercial production ofhigh toughness API-X80 grade hot rolled strips. ... C., USA, 1987. [20] V. A. Burnos, T. P. Vaschilo, and L.
  51. 2 Feb 2013: predictions [17, 20]. Table 1 is a compilation of published models describing the. ... neglected [18, 20] on the basis that it is smaller than that after coarsening.

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