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16 May 2024: Marquart, NJ Mason, C Mendoza, TJ Millar, N Moreau, SV Morozov, T Möller, HSP Müller, G Mulas, I Murakami, Y Pakhomov, P Palmeri, J Penguen, VI Perevalov, N Piskunov, J Postler,

16 May 2024: N Dorey, TJ Hollowood, SP Kumar, A Sinkovics. – Journal of High Energy Physics.

16 May 2024: Passvogel, G Patanchon, D Pearson, TJ Pearson, O Perdereau, L Perotto, F Perrotta, F Piacentini, M Piat, E Pierpaoli, S Plaszczynski, P Platania, E Pointecouteau, G Polenta, N Ponthieu, L Popa, ... B Partridge, F Pasian, G Patanchon, V Pavlidou, TJ

2 Sep 2012: 52 predicts for a single receptor if IJ = TJ(1 - p).

1 May 2020: Inverse ProblemsLecture notes, Michaelmas term 2019. University of Cambridge. Hanne Kekkonen and Yury Korolev. May 1, 2020. This work is licensed under a Creative Commons“Attribution-ShareAlike 3.0 Unported” license. 2. Contents. 1 Introduction

23 Jul 2016: Dηn‖2 ‖ζn‖2 t‖ζn‖. t(1 t)rj=0. tj(1 ρ(A). )[ j2](‖ηn‖ ‖ζn‖ ‖ηn1‖ ‖ζn1‖). ... en1‖ ‖Den1‖2 ‖ωn1‖2 ‖en‖ t‖ωn‖. ‖Den‖2 ‖ωn‖2. t(1 t)rj=0. tj[‖f(j)t. (U(tn).

16 Aug 2023: This. isasp. ecificindividual’scopyofthenotes. Itis. notto. becopiedand/orredistributed. Natural Sciences Tripos: IB Mathematical Methods I. Contents. Contents a. 0 Introduction i. 0.1 Schedule. i. 0.2 Books. ii. 0.3 Course Website. ii. 0.4

6 Oct 2014: Anti–self–dual fields. and manifolds. Moritz F. Högner. Trinity College. Dissertation submitted for the Degree of Doctor of Philosophy. October 2012. Abstract. Anti–self–dual fields and manifoldsMoritz F. Högner. In this thesis we study

16 May 2024: Ma, AJ Mungall, R Moore, MA Marra, MD Taylor, TJ Pugh, PB Dirks, D Strother, L Lafay-Cousin, AC Resnick, S Scherer, DL Senger, BD Simons, JA Chan, AS Morrissy, M

16 May 2024: no. 036. N Dorey, TJ Hollowood. – Journal of High Energy Physics.

8 Nov 2015: On the Solvability Complexity Index, the n-Pseudospectrumand Approximations of Spectra of Operators. ANDERS C. HANSENApplied and Computational Mathematics, California Institute of Technology,. hansen@acm.caltech.edu. Abstract. We show that it is

7 Apr 2017: Aus d e m Z o o l o g i s c h e n I n s t i t u t d e r U n i v e r s i t s H a l l e a. S.). Z U R T H E O R I E D E R F L I M M E R B E W E G U N G. ( D Y N A M I K , N U T Z E F F E K T , E N E R G I E B I L A N Z ). V o n. W I L H E L M L U D W

16 May 2024: AA Hamed, DJ Kunz, I El-Hamamy, QM Trinh, OD Subedar, LM Richards, W Foltz, G Bullivant, M Ware, MC Vladoiu, J Zhang, AM Raj, TJ Pugh, MD Taylor, SA Teichmann,

22 Nov 2011: Tj(x) = cos(j arccos x), j = 0, 1, 2,. ,. and c0 = 1π , cj =. 2π , j 6= 1. ... Given that the polynomials Tj are orthogonal with respect to the weight.

11 Dec 2017: Integrating this equation with respect to t, we find. TJ dV" d t.

22 Sep 2016: on September 22, 2016http://rsif.royalsocietypublishing.org/Downloaded from. rsif.royalsocietypublishing.org. ResearchCite this article: Marron AO, Chappell H,Ratcliffe S, Goldstein RE. 2016 A model. for the effects of germanium on silica.

14 Jun 2014: Development/Plasticity/Repair. Developmental Modulation of Retinal Wave Dynamics:Shedding Light on the GABA Saga. Evelyne Sernagor,1 Carol Young,1 and Stephen J. Eglen21School of Neurology, Neurobiology, and Psychiatry, Medical Sciences, University

16 May 2024: Quantization of Integrable Systems and a 2d/4d Duality. N Dorey, S Lee, TJ Hollowood. –

24 Sep 2002: 6- (/k; (6(tJ_6 &t Lxm.

16 May 2024: K Mason, A Masserot, TJ Massinger, F Matichard, L Matone, N Mavalvala, G May, N Mazumder, G Mazzolo, R McCarthy, DE McClelland, SC McGuire, G McIntyre, J McIver, K McLin, D

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

10 Apr 2011: J. Phys. II France 6 (1996) 767-796 MAY 1996, PAGE 767. Front Propagation in the Pearling Instability of Tubular Vesicles. Raymond E. Goldstein (), Philip Nelson (), Thomas Powers (>)and Udo Seifert (). () Joseph Henry Laboratory of Physics,

24 Jun 2014: On Asymptotic Incoherence and its Implications forCompressed Sensing of Inverse Problems. A. JonesUniversity of Cambridge. B. AdcockPurdue Univesity. A. HansenUniversity of Cambridge. Abstract. Recently, it has been shown that incoherence is an

6 Nov 2019: uj = Φ1(tj) = erf. 1(. tj. α. 2. ),. where tjs are drawn randomly from the uniform distribution U([0, 1]). ... Let us discretise theinterval [0, 1] by points tj = j/N and write uj = f(tj).

2 Sep 2012: CURRENT TOPICS IN PLANT RESEARCH. The sliding theory of cytoplasmic streaming: fifty yearsof progress. Teruo Shimmen. Received: 18 August 2006 / Accepted: 22 November 2006 / Published online: 25 January 2007! The Botanical Society of Japan and

13 Apr 2011: F(x) = 12xT{ n. j=1 100(j1)/(n1) vj v. Tj. }x, xRn.

22 Jul 2010: K. = 0, v.3. gij = (1 t m , m ) s i j - tj,i k i j ,. F = - t+ xi (P9p 99. (2.10). where k i j is the ( i ,

27 Nov 2011: THE ROTARY MOTOR OF BACTERIALFLAGELLA. Howard C. BergDepartment of Molecular and Cellular Biology, Harvard University, 16 DivinityAvenue, Cambridge, Massachusetts 02138; email: hberg@biosun.harvard.edu. Key Words Escherichia coli, motility,

12 Aug 2016: J. Fluid Mech. (2013), vol. 722, pp. 554–595. c Cambridge University Press 2013 554doi:10.1017/jfm.2013.122. Invariant recurrent solutions embedded in aturbulent two-dimensional Kolmogorov flow. Gary J. Chandler and Rich R. Kerswell†. School of

10 May 2022: travel back to the position where they originated. Because Fj and Tj are the forces and.

13 Jul 2009: x(tj-(O)]=n6D,Ati=2D,t, (24). where the factor l/3 represents the variance of a random number chosen uniformly on [ - 1, 11.

31 Oct 2023: a) Prove [ti , tj] = iǫijktk. (b) Prove (nt)3 = |n|2nt.

30 Oct 2010: MECHANICAL PROCESSES IN BIOCHEMISTRY. Carlos Bustamante,1–3 Yann R. Chemla,3. Nancy R. Forde,1 and David Izhaky11Howard Hughes Medical Institute and the Departments of 2Molecular and CellBiology, and 3Physics, University of California, Berkeley,

10 Apr 2011: Continuum theory of critical phenomena in polymer solutions: Formalism and mean field approximation. Raymond E. Goldstein Laboratory of Atomic and Solid State Physics and Materials Science Center, Clark Hall, Cornell University, Ithaca, New York

2 Jun 2016: 23. where we definet̃i = εij tj , ̃i = εijj , (7.3).

22 Aug 2012: whereas the response to a force at a latitude equator- ward of that given by the right-hand side of (9) appears primarily as an acceleration, O tJ/Ot, rather than

19 Nov 2008: Prove the results (a = |a|),. (i) [Ti , Tj ] = iijkTk ,. (ii) (aT)3 = a2aT ,. (iii) exp(iaT) = 1 iaT sin aa (aT)2 cos a1.

1 Sep 2011: x) : 1(yi1) = g(yi1); 01(yi1) = g0(yi1+);ki1(x) : ki1(yi) = g(yi); 0ki1(yi) = g0(yi);and for j such that Tj = Tj ,j(x) : 8><>: (r)j ... Hence 2 S(A0i;1); A0i 2 Xj: Tj=Tj 1:Since i(x) = maxf(x); p(x)g;we change into p at most once in each T j.

24 Sep 2014: Define structure constants by [Ti,Tj] cijkTk. Antisymmetrysays cijk = cjik c(ij)k = 0. ... Now computing the nested brackets gives:. [[Ti,Tj],Tk] = cijl[Tl,Tk] = cijlclkmTm.

27 Jan 2012: Forcr = 0 show that det AN = N 1. If D(tj ) = det Aj show that as N we have.

16 May 2024: JM Evans, TJ Hollowood. – Nuclear Physics B. (1997). 493,. 517.

5 May 2015: We define Fk. j1 Tj as the set of all trees of power k in h which appear.

6 Oct 2011: 52 predicts for a single receptor if IJ = TJ(1 - p).

21 Jul 2009: http://journals.cambridge.org Downloaded: 21 Jul 2009 IP address: 131.111.16.227. 3. Fluid Mech. (1993), vol. 256, pp. 3 4 3 4 0 1 Copyright @ 1993 Cambridge University Press. 343. Nonlinear drift interactions between fluctuating colloidal particles:

10 Nov 2016: The Evolution of Silicon Transport in Eukaryotes. Alan O. Marron,1,2 Sarah Ratcliffe,3 Glen L. Wheeler,4 Raymond E. Goldstein,1 Nicole King,5 Fabrice Not,6,7. Colomban de Vargas,6,7 and Daniel J. Richter5,6,71Department of Applied Mathematics and

13 Dec 2018: dx8,. Tj ,n5 2 Exj 21. ... xjGr1;r28!dx8,. Sj ,n8 5 Exj 21. xjGr2;r18!dx8,. Tj ,n8 5 2 Exj 21.

2 Nov 2007: "# $%& '&(),#-.(/ 0&&1&. 243563798:3<;>=?A@CBD7FEG. HJICKMLONCPRQOLSUT#VXWJYJZ[]_]_Facb dMefWhgi]jDbkbCW1limCend_bk[oefoXpqb d_]rq[DpXb sCtendbk[oO]efZW#mX]_Wpud_[W1vkmXt1bkpCendWwpXb

6 Dec 2020: On the infinite-dimensional QR algorithm. Matthew J. Colbrook† and Anders C. Hansen†. †DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Rd,Cambridge CB3 0WA, United Kingdom. Abstract. Spectral computations of

2 Dec 2021: i. {avgj. ([Re(tj) RΞi (gtj)]. 2)}. i. , (S2). where i iterates over all datasets and j over all pointswithin the experimental dataset Re(tj) = Re(tj)/Re(0)enumerated by ... avgj. ([Re(tj) RΞ (gntj)]2. ). (S3). Here, all minimizations were performed

10 Feb 2010: Pn3 y. Cn3|. 29. Let p be the cubic polynomial that is defined by p(tj ) = yj , j = n, n 1, n 2, andby p′(tn2) = f (tn2, yn2).