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5 Dec 2012: γ+ su(2) self–dual YM on (M,g) Skyrmion on M/SO(2). A = (1/2)εijkγij tk, where [ti,tj] = εijktk.AH, Taub–NUT, CP2 are SO(3) invariant.

22 Aug 2012: 40C to 125C. Junction Temperature (TJ):. 150C. ESD Protection On All Pins (HBM:MM):. ... Note: Operation in this range must not cause TJ to exceed Maximum Junction Temperature (150C).

15 Aug 2012: n,(c) if ti = tj , then (ti, zi) / (tj , zj ) in {ti} Zd, for 0 i < j n.

26 Jun 2012: t!fsA b =. jJB(tj, b). iI. [J(j, fi) A(si). ]. Examples:.

2 Sep 2012: The Mechanics and Statisticsof Active Matter. Sriram Ramaswamy. Centre for Condensed Matter Theory, Department of. Physics, Indian Institute of Science, Bangalore 560012,. India and CMTU, JNCASR, Bangalore 560064, India;. email:

27 Oct 2012: Viterbi Algorithm (for a bigram tagger) 17. δtj (n 1) = maxtiδti(n)P (ti|tj)P (wi|ti). ... where δtj (n1) is the probability of the most probable tag sequence endingin tag tj at position n 1. •

27 Jan 2012: The outcome is a decomposition ofγ into an ordered set of bridges with vertical displacements written T0 > T1 > > Tj. ... Therefore,. Z(x) 2. Ti<<T1T0>>Tj. j. k=i. ζxTk = 2. T =1.

6 Jun 2012: Cop. yrig. ht. 201. 2 U. nive. rsity. of C. ambr. idge. Not. to b. e qu. oted. or. repr. oduc. ed w. ithou. t per. mis. sion. Part II Mathematical Biology Lent Term 2012. lecturer: Professor Peter Haynes (phh@damtp.cam.ac.uk). May 31, 2012. These

16 Feb 2012: l1]Tj. Cambridge UniversityEngineering Department. MPhil in Advanced Computer Science 10. Module L101: Machine Learning for Language Processing.

15 Aug 2012: t0,x0,. ,xr1, tr) for some r 0 with xi Z2{O}, ti T, and tj 6= R for. ... iii) r = s 1, xi = yi for i r 1, tj = uj for j r, ys O and us = R.