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7 Jun 2010: 35T;w38s35/2NQRD2/2A.8;-0:K/l$N2O8HN2-7=;?%603nLK+@=X<h+.=>QR:K=>aOTX360-7/2n3G={A@:Ka]42-0/F3t8H-0:5/q:5Q&n35AsN$N2-0?2?P+@/vD2/ ... J8HGl -7IK+./d8HNF3G88;N2+<@=;T>:K/9?2=H3niST8H-0a9+@TyR=;.<26z35A.-0/21_8;N2+4F356760T#:5/O+@35AsNO:fA@A@35T;-7:K/»QR=>

7 Jun 2010: The specific values of kA and n depend on the natureof nucleation and growth. ... p. 216. Table 3 Values of ln kA for each crystallisationtemperature from normalised data.

7 Jun 2010: Substituting for ψ(x) we get: A sin kaB cos ka = 0 (1). ... A sin kaB cos ka = 0 (3). Adding equations (1) and (3) gives: 2Bcos(ka) = 0.

12 May 2010: Institute/Li Ka Shing Centre; Faculty of Education; Institute of Criminology;Department of Chemistry (Photo: Nathan Pitt); Institute for Manufacturing; Kavli Institute forCosmology at Cambridge; Wellcome Trust and Cancer Research UK

4 Apr 2010: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971).

7 Jun 2010: force of 1.69 kN and a peak current of 8.1 kA. ... a) (b). (c) (d). Figure 3: Resistance spot weld produced using interstitial–free steel with 7 kA current, 30 cyclesweld time [3] (reproduced with permission of B.

8 Apr 2010: 210). for some one–form Ka. Note that (210) follows from (28) withK A A′ = ω B′A′ ϒB′ A, (211). ... Then (29, 210, 215) must hold with. constant , in which case Ka vanishes but from (215) we deduce = 0 ; φA B A′ B′ = ωA′ B′ ρA B.

29 Oct 2010: It is housed in the Li Ka Shing Centre, a state-of-the-art research facility located on the Cambridge Biomedical Campus which was generously funded by Hutchison Whampoa Ltd, Cambridge

7 Jun 2010: "!#$&%')(,%-./' %0( 12(/304$65798:$&'. <;4=. 2>?%0$A@B.23DCE7F@F@G(H $&@9IJ!LK B(M@F@G$ONP$:QLRSK798M$A'D3T79C!(2U"BV./WYX' 7F%0NP$. ;S$&Z./'[CEW<$AKPC(2U]. C_$&' 7F.P@G3 Ha 7G$&K $?/K% $bCE.P@F@F-')N2!#$&WYX')(Mc2$ H CE'D$d$bCQLB.PWYX' 7F%0N/$?B egf

7 Jun 2010: 5. 6. 7. 0 1 2 3 4 5 6 7 8Post heating current, kA. ... 10. 15. 0 2 4 6. Post heating current, kA. Max.

4 Jan 2010: The advent of new technologies has enabled researchers to interrogate human genomes at unprecedented resolution. These technologies have led to a wealth of

7 Jun 2010: ξ = 1 exp{kaG3It4}. where ka is a constant.[40%]. END OF PAPER.

4 Jan 2010: For more information, please contact Professor Kevin Brindle (kmb1001@cam.ac.uk) at the Department of Biochemistry and the Cancer Research UK Cambridge Research Institute/Li Ka Shing Centre.

7 Jun 2010: " #%$&')( ,.-0/%12)354567/%892:-.

7 Jun 2010: b 0.15 15. c 0.4 80. ka. = 100. 0.1. (1 11 1. ). =.

7 Jun 2010: #"%$'&)(-,/.10324(5/(6&. 157285%9%2;:<289%=>.6?A@>.6B0C24DE?4$F285G:(?;:$IHJ2;0CH#5K=%DI?8$L.10324(57.65M9N+-(PO#0C"RQSTN+(U(<9V03"%$IXW,Y(<9MZU5>.1,[28D'9%$IH-DI328@M0C28(5(6&0C"%$]@%">.6H-$IHF285K:6(?8:6$I928H_$EH3H3$E5G0C2.1?245(39M$IJ0C(V,Y(<9M$I

21 Jun 2010: In metallic tubes, the LO mode is affected by a Kohn anomaly (KA) [43, 44], which causes the softening of this phonon [43, 44]. ... Since KA are not present in semiconducting SWNTs, the G+, G– assignment in metallic SWNTs is the opposite of

7 Jun 2010: #"%$'&() ,.-/ 01324"653"78"29"%$.&5:,.,. ;<" =&>?@A.24"B9" =&5CDE%-/-/F!GH" I$7J,.KD/LM,.)FNOPD,Q01DESR@T.0%,.T.,CD,UVE%E%DW&XY0%Z[,U-/0]WFDNO_L8a60b+,&X4" 5= 7Y,.K'/LM,.cFNd;Se6Kf,U0%LM,.VEhgd @W6-/0%T.-.&_) DEbLM,Q-iX?0%Z[,U-/0jWkFDNdlm,.TV

29 Jul 2010: cal g- 1 o C- 1 apr 0.380 cal g- 1 o C- 1 ka 0.008 cal cm -1 s -1 øC-1 k•5 0.008 cal cm -•

7 Jun 2010: Bibi ka Maqbara (Wife’s tomb), Aurangabad byAurangzeb. Discover : Europe To India_/0.%k.

7 Jun 2010: ξ = 1 exp{kAtn} (2)where t is the time, kA and n rate constants and ξ is given by.

18 Feb 2010: 17  6  23  23 2002  100  16  7  23  23 2004  100  17  5  22  22 Source: GOUP: Vidhan Parishad ke Sadasyon ka Jeevan Parichay, UP Vidhan Sabha Sachivalaya, 2004, ... Sources: Table computed on the basis of information in: (i

19 Jul 2010: cal g- 1 o C- 1 apr 0.380 cal g- 1 o C- 1 ka 0.008 cal cm -1 s -1 øC-1 k•5 0.008 cal cm -•

11 Nov 2010: Nature 413:39–44. 3. Aylett CHS, Wang Q, Michie KA, Amos LA, Löwe J(2010) Filament structure of bacterial tubulin homo-logue TubZ.

29 Jan 2010: y0! (R0iig Symk F)x! (R1g! Symk F)x! (R1g Symk F)x! 0k k kA B CHere the top line is the exact sequence (2.8.1), and the bottom

7 Jun 2010: 1!ÁCT "'/;:Âm 89 ";JG_uG15ÿ- "%;, "(LG:;1!_,!;U!];U.5%:1T LP@1ULN1:1'FYF01%:ÄqÅv5H1@¿- "!Æ1:GoY['W%.X%YF%%0=1!1!=."6!0" ... 1¿1GWPu ";iX!1P@ "6Y[.%U18ZG kA"G.Z 1 %5<"1'( U.1!5i Z1!5G7Hk8y5H:4"15GsX%GuC31: "{¿$15V6T2-1!:¿$1%ÂqrU%0=1 ":VE.

19 Mar 2010: Bone 14(Suppl 1):s51–s56. 53. Dretakis EK, Steriopoulos KA, Kontakis GM, Giaourakis G,Economakis G, Dretakis KE 1998 Cervical hip fractures donot occur in arthrotic joints.

14 Dec 2010: dUOncology, Li Ka Shing 2007 brUce aNTHoNy JoHN poNder, JEOperations Research 2007 daNiel ralpH, CHUOphthalmology 2010 keiTH roberT graHam marTiN, CTHOrganic Chemistry (2001) 2001 iaN paTerSoN, JEOrganic Chemistry, Herchel Smith VacantOrthopaedic

11 Oct 2010: Alloy Current, kA Nugget, mm. Tensile shear strength Cross-tensile strength. Maximum load, kN Fracture Maximum load, kN Fracture.

7 Jun 2010: ξ = 1 exp{kAtn} (2). where t is the time, kA and n rate constants and ξ is given by.

8 Jun 2010: Neuron 40:177–188. Bernander O, Douglas RJ, Martin KA, Koch C. 1991.

7 Jun 2010: phenomena. 1Magnetic field / kA m. 3. 01.5 0R. MS. Bar. ... ltage. / V. Applied field / kA m. Figure 4.15: Change in the shape of the BN signal from as-quenched ().

7 Jun 2010: eff. nf Ka. vFfT. = (15). For f the appropriate coefficient of friction from the wear regime applicable for the specific summitshould be used (Eqs.

7 Jun 2010: X-ray experiments were conducted using a PhilipsPPW1730 diffractometer and a scanning rate (2q ) of1 min1, with unfiltered Cu Ka radiation.

7 Jun 2010: The amount of retained austenitein the hot rolled samples36 was determined usingquantitative X-ray analysis on a Phillips X’Pert dif-fractometer and unfiltered Cu Ka radiation.

7 Jun 2010: X-ray experiments were conducted using a PhillipsPPW1730 diffractometer and a scanning rate (2q ) of0.1 min1 over the range 2q =30–110, with unfilteredCu Ka radiation.

7 Jun 2010: TRIP800. DP980. X-IP 1000. X-IP 1000Rephos. 280. Current (kA). Fig. 7.

7 Jun 2010: Steel 1 / steel 2 (thickness, mm) (coating). Welding data1). I2) (kA).

29 Sep 2010: F5?G0RH! '&%FA%F5 RH!03"!VRCaOBs5?"! XBUc5?CWn!V/>P(!(3]5?%&'F! Q.):9 Q.%F3]5>!(/w5>0QJ3G { Q 7:g,-!(b@!(/8D5?"!KA!8RH%QJ3jAjQJZ@3"% ... 8R}9;/>,.A %F5>)$)?VP(,.30RHy ,@/>RH!V/KA,.A!V3@5i)(7 "%)YnQJZAjQJ3nQJZ!8)l5?,!('&%FA%&30Qc5>!$A,@)E5K)EW"G0/?%&,.G0)-

25 Feb 2010: Kernel Methods forText-Independent. Speaker Verification. Chris Longworth. Cambridge University Engineering Departmentand. Christ’s CollegeFebruary 23, 2010. Dissertation submitted to the University of Cambridgefor the degree of Doctor of

7 Jun 2010: 20. 40. 60. 80. 100. 0. 1. 2. 3. 4T. i Ka.

29 Jan 2010: INDEX TO SGA 1. INDEX TO SGA 1! " # $ % & $ ' & " ( # ) # # & , -! / #! 0 ' %! 1 2! 3 , -! / #! % / 2 # )! ' #! 4 , -! / #! # ) % & #! 5 # 6 # 7 # / #! # ) % & #! 38 9 % - - # ) # ) : " % / # % & # " #! / -! / #! # ) % & #! 8; < - - & $ % % ' = # = #

7 Jun 2010: They were then step-scanned in a SIEMENS D 5000 X-ray diffractometer using unfiltered Cu-Ka radiation.

7 Jun 2010: FHGJI(K8F GJIML N O PRQ F GJIML NSUT@O PVQ F GJIML N O P;SCTKXWYHZ [ Q [HZ]W2 Q [_Ka"Z6b"W ¡c L.

7 Jun 2010: FHGJI(K8F GJIML N O PRQ F GJIML NSUT@O PVQ F GJIML N O P;SCTKXWYHZ [ Q [HZ]W2 Q [_Ka"Z6b"W ¡c L.

7 Jun 2010: ξ{t} =1 exp{kAtn}. with ξ{t} = H0 H{t}H0 HF. and kA = k0 exp. {

13 Oct 2010: 2008 Mr Graham Clapp. 2009 Dr Stephen Blyth. Honorary Members. 1999 Sir Li Ka-Shing KBE.

13 Nov 2010: Annu. Rev. Biophys. Biomol. Struct. 1996. 25:395-429 Copyright 0 I996 by Annual Reviews Inc. All rights reserved. VISUALIZING. INTERACTIONS ON A LARGE SCALE WITH THE SCANNING FORCE MICROSCOPE. PROTEIN-NUCLEIC ACID. Carlos Bustamante" and Claudio

30 Dec 2010: By. are shown in Fig. 3. They are related by kAy kBy = 2π α.1Hence, cos(kA(B)y ) = cos(kB(A)y 2π α), so the Hamiltonian (8)is the ... 1Note that the positions kA(B) of these minima are gauge dependent.

7 Jun 2010: with unfiltered Cu Ka radiation, and the systemoperating at 45 kV and 45 mA.