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1 - 10 of 17 search results for KA :PC53 |u:www.damtp.cam.ac.uk where 0 match all words and 17 match some words.
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  2. How to recognize a conformally Kählermetric Maciej Dunajski…

    www.damtp.cam.ac.uk/user/md327/Kahler_leeds.pdf
    20 Sep 2011: ω 6= 0 so ω defines a Killing vector Ka.Killing identity Ka RabKb = 0, where Rab = gab/4. ... M|K|2gd4x = 1. 4. M|K|2gd4x. Therefore Ka = 0 and our assumption was wrong.
  3. PII: 0378-4371(89)90400-7

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/lekkerkerker.pdf
    10 Apr 2011: 2 6 ) - ( 2 8 ) to order 1/(Ka) 2 the following expression for the surface potential:. ... 1 2 ( q - 1) 1 ( q - 1)2(2q 1) 3 3 , (29) = 2 l n ( p q) Ka p q ( K a ) 2 p q.
  4. Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…

    www.damtp.cam.ac.uk/user/gold/pdfs/trapping.pdf
    10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de
  5. Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments…

    www.damtp.cam.ac.uk/user/gold/pdfs/teaching/trapping.pdf
    10 Apr 2011: Trapping and Wiggling: Elastohydrodynamics of Driven Microfilaments. Chris H. Wiggins, D. Riveline,# A. Ott,# and Raymond E. Goldstein. Department of Physics, Princeton University, Princeton, New Jersey 08544 USA; #Institut Curie, Section de
  6. 20 Jan 2011: 2.12)Consider a complex tetrad of 1-forms. Ka = i(α̂AβA′ αAβ̂A′ ), Xa = α̂AβA′ αAβ̂A′ , Za = αAβA′. ... We now use(2.16) to find. φAB = 2|K|2 KA′B AA′. (1.
  7. dblp.dvi

    www.damtp.cam.ac.uk/user/na/people/Alexei/papers/dblp.pdf
    1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is
  8. SHA.dvi

    www.damtp.cam.ac.uk/user/na/people/Alexei/papers/dmrus.pdf
    1 Sep 2011: TO KA-SAETSQ PORQDKA POLIGARMONINOSTI (g) = @(f)=@xj, TO, POSKOLXKU OPERACIQ DIFFERENCIRO-WANIQ SOHRANQET TOT PORQDOK, IMEEMr2(g) = 0; = m1 1 2m1 = m:pREDLOVENIE 1a0, A S NIM I SLUAJ 1a)
  9. Theory of multiple phase separations in binary mixtures: Phase ...

    www.damtp.cam.ac.uk/user/gold/pdfs/JChemPhys_78_1492.pdf
    10 Apr 2011: 3). vs T = - l/Ka• Recall that this expression refers to the formulation in Eq. ... I(K1,K2 ,Ka) =! Ko+ In Tria,) exp[L: Keff(l- Oa,a /)] , (lJ) (16).
  10. doi: 10.1098/rsta.2010.0225, 2133-2147369 2011 Phil. Trans. R. Soc. A …

    www.damtp.cam.ac.uk/user/mem/wolff-phil-trans11.pdf
    5 Aug 2011: Although the strong correlationsuggests an almost constant and linear relationship, it actually appears as ifthe earliest part of the record (before about 650 ka) had lower mixing ratios(both absolutely and ... a) The last interglacial and methane. The
  11. RAPID COMMUNICATIONS PHYSICAL REVIEW E AUGUST 1997VOLUME 56, NUMBER…

    www.damtp.cam.ac.uk/user/gold/pdfs/PRE56133097.pdf
    10 Apr 2011: RAPID COMMUNICATIONS. PHYSICAL REVIEW E AUGUST 1997VOLUME 56, NUMBER 2. Elastohydrodynamic study of actin filaments using fluorescence microscopy. D. Riveline,1 C. H. Wiggins,2 R. E. Goldstein,3 and A. Ott1,1Laboratoire PhysicoChimie Curie,†

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