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6 Feb 2019: Conf [J ] = KJ Lor (J ) D TJ. Lor (J ) is the 5D U-duality group that leaves the cubic norminvariant.

25 Feb 2016: FL48CH05-Lauga ARI 24 November 2015 12:50. Bacterial HydrodynamicsEric LaugaDepartment of Applied Mathematics and Theoretical Physics, Center for MathematicalSciences, University of Cambridge, Cambridge CB3 0WA, United Kingdom;email:

21 Feb 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

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.

18 Jul 2024: TJ Pugh, MD Taylor, M Hirst, CJ Eaves, BD Simons, PB Dirks. –

18 Jul 2024: Montier, G Morgante, A Moss, S Mottet, M Münchmeyer, P Natoli, HU Nørgaard-Nielsen, CA Oxborrow, L Pagano, D Paoletti, B Partridge, G Patanchon, TJ Pearson, M Peel, HV Peiris, F

1 Sep 2011: More details on the problems relevant to k;p can befound in [1],[2],[5].Recall that Nj(t) := (tjk tj) [tj; tj1; : : :; tjk] ( t)k1+ ;so that suppNj = (tj; tjk); ... degree p such thatsuppMj;p = (tj; tjp1); Z tjp1tj Mj;p(x)dx = 1;and by!

18 Jul 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,

24 Feb 2005: ωw0,.,wn (tj; tj)> 0. PROOF. We omit to write the weight functions wm here as well. ... Thus,. α. ε=ω(tj; t(ε))ε ω(tj; tj). ε0. ω′(tj; t). ω(tj; tj).

24 Nov 2006: K} such that. ti º tj , j = 1, 2,. , ... K. If ti tj for all j 6= i, we let (ti, ti1,. ,

1 Sep 2011: 2. Condition number and related constantsLet fN̂jg be the B-spline basis of order k on a knot sequence t = (tj), tj < tjk,normalized with respect to the Lp-norm (1 ... p 1), i.e.,N̂j(x) = (k=(tjk tj))1=pNj(x);where fNjg is the B-spline basis which

18 Jul 2024: N Dorey, TJ Hollowood, D Tong. – Journal of High Energy Physics.

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

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

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).

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

18 Jul 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

18 Jul 2024: HY Chen, N Dorey, TJ Hollowood, S Lee. – Journal of High Energy Physics.