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20 Nov 2009: 82. 82 P. bLe. ad20. 7.2. 7.41. 67. 83 B. iBi. ... 5.89. 97 B. kBe. rkeliu. m(2. 47). 6.19. 79. 98 C.

29 Jan 2009: the direction of the normal b, |b| = 1 to the plane,is arbitrary. ... We get. (B+ B).tl = µ0s.bl. (B+ B).n b = µ0s.b.

21 Jan 2009: B[p] := {bp : b B}. in B provided that B is reduced.Let t be a positive integer. ... Hence ι is surjective. Because b. p B1 for all b B, we see that ι is injective.In fact, it is easy to see that the inverse of ι is

28 Jan 2009: α β γ = π A(). 4. A. A. B. B. ... A Bu. C. v. C. B. α. Corollary 2.8 Spherical Cosine Rule II.

16 Oct 2009: of the form6 Z =. [b ca b. ]. Let us consider the map given by. ... 0X1t Et Xt dt. Write A :=[b ca b. ]. We have to prove that.

23 Jul 2009: find that it is not necessary to know the tensors A , B and C in full detail, because the final answer only depends on the combination. ... w - [G+&A-l.B : B T A - l G ]. p(4.rcvt)$ vt. Finally we recall t h a t the angular-velocity autocorrelation

9 Sep 2009: The Role of Mobile Technology in Learning and Teaching Swarnalata Harichandan, H.B.B.Ed College, India Integrating New Technologies in Management of ODL Institutions: Experiences of the University of Mumbai

28 Nov 2009: e.g. : only one possible exchanged gluon. b b. b b. ... b b. Configurations where quarks swap colours. gr. g r. Appendix II: Colour Potentials.

20 Feb 2009: Another line ncrosses at a (movable) point B and a fixed angle β. ... cos α =cosh b cosh c cosh acosh2 b 1. cosh2 c 1.

24 Nov 2009: checks // : Clone shared photon track hits // : new photon recovery structure // : removed some obsolete and unhelpful code // 20/6/2007 : Add PerfectPFA // CVS1.6 : get B-field from global // : allow possibility of