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28 Nov 2006: limx. µx2 1. x 1ax b. = 0,. what should a and b be? ... c) Find a basis for Null(A) and Col(A). (d) Find a basis for the following set B = {b R4 | Ax = b has nosolution}.

31 Jan 2006: O. é{ê_êcë¥ìë¢íî_ïðKñzò_óôìë¢íî_ôOO WZnWYXZY}YwXr|.qRqXERq}fYasd eYfvWYX> ][w >qWYXmO KKI|.0X}d efpcv ][w nKRaWhX}uowuqRqusoaZnÝ 4e|Yd ef_o{uY4Rx[w RqdQWs dexXr >XuRqvr_b.

27 Apr 2006: o c k e d b y r u b b l e a n d previous- ly c o o l e d lava. ... p a n d s t o f o r m t h e r u b b l y surface.

12 May 2006: trivially embed this in the non-abelian theory. B= B?0.( 0( ((q =q? ... B? q? SU(N)diag/SU(N 1) U(1) = CPN1. Simple Idea:. The strings can miss each other in the internal space.

23 May 2006: Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(. ... A. B. ). where. a = 81α/(1 144α2) and b = 3(5 72α2)/2(1 144α2).

15 Sep 2006: Finally (1) and (4) can be written. d r b 4/3 _,d t b b I b b - b •. Equations (8)-(l 1) describe the heat transfer and melting process ... a). 50 100. b). 100. c). 50 100. TIME (yrs). F I G.

1 Jun 2006: A A A (1 A) and A (1 A) =. (ii) |A| = min{|B| : A B (1 B)}.(iii) |A| = max{|B| : B A,B (1 B) = }. Proof: (i) We may assume ... B : B Z/nZ, |B| = r 1,B (1 B) = }. In particular I(SecrΓn) is generated by a space of (r 1)-ics of dimen-sion β(r 1,n).

19 Apr 2006: F! a! TS- '4( );V! (Y C( E5[- M(&? 3$ (49 P#-# -;9!9]%& W5[- ; ) Ea'-'; UG4?3$ )9&$ B ; B- t%3 ,:E# ;! 5- t(&$7C0:; P B 'RS! ... G. u= K G %' àõö>øEàù ú»s6ø 6þC.ø?»ý ø @2& B B- u 7:>- ra%. (&

26 Apr 2006: where. B"B(j, hi)"! hi. Jpej2@4erf(j/2). (35). Eq. (34) is the transcendental equation determin-ing the eigenvalue j. ... Since gH is independent ofhiand B is expressed in closed form, we can calcu-.

1 Nov 2006: C. KENNICUTTAstronomy and Geometry, Lowndean 2000 B. J. TOTAROAstrophysical Fluid Dynamics 2000 M. ... C. WOOD, GAncient Philosophy 2001 R. B. B. WARDY, CTHApplied Economics 2002 J.