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4 Feb 2020: Then for each time interval tj–tj 1 with1ojoM, predictions of the beach profile for tj 1 were made usingK̄(x)k in place of K in Eq. ... 14) can be written as. hðxi; tjþ1ÞffiðexpðDtÞ 1ÞD1GþexpðDtÞhðxi; tjÞ ð15Þ. where t= tj 1tj.The

4 Dec 2020: Mostofi, AA. Hamp, J. Harris, WA. Zuehlsdorff, TJ. Cheng, C. Lin, LH.

5 Jun 2020: trace(Qtj h(y))w(y)w(y). T= O(V (y)2e(tj)); j = y 2 X:. Similar reasoning may be applied for arbitrary k;j, and this shows ... o dened by linear interpolation on theremainder of [Tj;Tj1] to form a piecewise linear function.

20 Jan 2020: random variables, independent of N. Show that if g(s,x) is a function and Tj are the. ... E. expθ. Ntj=1. g(Tj,Xj).  = exp {λ t. 0. [E(eθg(s,X)) 1.

4 Feb 2020: RANDOM PLANAR GEOMETRY, LENT 2020, EXAMPLE SHEET 1. Please send corrections to jpmiller@statslab.cam.ac.uk. Problem 1. (i) Show that the cardinality of the set Tk of plane trees with k edges is the kth Catalan number. Ck =1. k 1. (2kk. ). [Hint:

19 Dec 2020: p.53, line after (2.55), replace second ‘|λi|’ by ‘|µi|’.p.57, line -8 to -2: it should read i) ‘d(ti, tj) ε’ (missing comma), then ii) ‘= ε2/2 ... d2X(ti, tj)’.

24 Aug 2020: i=1R. j =1 E(τi )Ti Tj τi τ2j (τj τi )R. ... 20 R. k=12k. [E0. E(τk ). ]2. = 4C2R. k=1Tkτk. [ Rj =1 Tj τ.

8 Jun 2020: FtsK in motion reveals its mechanism fordouble-stranded DNA translocationNicolas L. Jeana, Trevor J. Rutherforda, and Jan Löwea,1. aStructural Studies Division, Medical Research Council Laboratory of Molecular Biology, Cambridge CB2 0QH,

13 Oct 2020: C O P i Lc a m b r i d g e o c c a s i o n a l p a p e r s in l i n g u i s t i c s. Volume 6, Article 7: 201–236, 2012 | ISSN 2050-5949. SUBJECT AGREEMENT AND THE EPP IN. BANTU AGREEING INVERSION. j e n n e k e v a n d e r w a l. University of

5 Oct 2020: 2. The Integer Quantum Hall Eect. In this section we discuss the integer quantum Hall eect. This phenomenon can be. understood without taking into account the interactions between electrons. This means. that we will assume that the quantum states