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shadrin.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/mon.pdf1 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. -
revision.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/kmon.pdf1 Sep 2011: f (tj ) = g(tj ) on {a = t0 < t1 <. < tn < tn1 = b}. Then, there exists a spline z such that. ... be such thatg(tj ) = p(tj ) on {a = t0 < t1 <. < tn < tn1 = b}. Then, there exists a spline z such that. -
Representation Theory Lectured by S. Martin Lent Term 2009, ...
https://www.dpmms.cam.ac.uk/study/II/RepresentationTheory/2010-2011/Representation_Theory.pdf12 Jul 2011: Representation Theory. Lectured by S. Martin. Lent Term 2009, 2010, 2011. 1 Group Actions 1. 2 Linear Representations 3. 3 Complete Reducibility and Maschke’s Theorem 7. 4 Schur’s Lemma 10. 5 Character Theory 13. 6 Proofs and Orthogonality 17. 7 -
Pub lishe d by Man ey P ublis hing ...
www.phase-trans.msm.cam.ac.uk/2002/Widmanstatten.pdf6 Nov 2011: It follows that. fMs'La = v{}'L-M Tj v{T} dT. (20)Figure 1 of Ref. -
ppat.1002260 1..9
www.jiggins.gen.cam.ac.uk/pdfs/longdon2011c.pdf26 Sep 2011: Host Phylogeny Determines Viral Persistence andReplication in Novel HostsBen Longdon1,2, Jarrod D. Hadfield1, Claire L. Webster1,2, Darren J. Obbard1,2., Francis M. Jiggins3. 1 Institute of Evolutionary Biology, University of Edinburgh, Ashworth Labs -
PII: 0198-0149(81)90135-7
www.itg.cam.ac.uk/people/heh/Paper41.pdf26 Sep 2011: tJ l,t,R. occupied with the failing conductivity cell and Stas S842 to 8853 with the r c p l a c c m e u resistor. -
Physics of chemoreception
www.damtp.cam.ac.uk/user/gold/pdfs/teaching/bergpurcell.pdf6 Oct 2011: 52 predicts for a single receptor if IJ = TJ(1 - p). -
PHYSICAL REVIEW E 83, 031306 (2011) Shallow granular flows ...
www.itg.cam.ac.uk/people/heh/Paper226.pdf13 Apr 2011: i. j. [h(xi ,tj ) f (xi ctj )]2, (2). where h represents the thickness recorded at discrete positionsxi and times tj. -
Phenomenological theory of multiply reentrant solubility Raymond E.…
www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_83_1246.pdf10 Apr 2011: tJ.Se(T,Hcrit ) = Se(T,H--Hcrit ) - Se(T,H--Hcrit -). (17). where.tJ.Ms is the order parameter jump of the SM. ... tJ.Me(T ,Hcrit) = Me(T ,H--Hcrit ) - Me(T ,H--Hcrit -). (18). -
PART II REPRESENTATION THEORYSHEET 3 Unless otherwise stated, all ...
https://www.dpmms.cam.ac.uk/study/II/RepresentationTheory/2010-2011/repex3.pdf24 Jan 2011: tr](this means that σ is a product of disjoint cycles of length t1 > > tr where n = t1 tr,and some of the tj may be equal to 1.
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