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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.

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).

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.

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

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

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: 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.

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

7 Jun 2010: AGaHsp.1Z>DF'8. çcã_èS62T C ßÈD>89C):7<f;54[&(.ÏU@VFRßir/Zõ5qSa-AWFTUòZR,07d<f;54(LK]ka@VFõ/o5r/r ... t,?õ5q/r Ø

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: 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

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

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.

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

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 -•

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

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.

12 Aug 2010: Service intervals are at about 500,000 pulses. The discharging currents vary, depending on the model, between 100 and 2000 kA.

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.

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: 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: 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: 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: 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.

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.

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

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: Steel 1 / steel 2 (thickness, mm) (coating). Welding data1). I2) (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: 20. 40. 60. 80. 100. 0. 1. 2. 3. 4T. i Ka.

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 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

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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.

7 Jun 2010: 3. 1ij ik kj. ka b c. =. = would use do loops both to perform the summation over k, and to run over all the values of i and j, setting each

7 Jun 2010: due to even a single pulse treatment. At current density up to 10.5 kA/mm2 and. ... 10.5 kA/mm2; pulse duration 130μs [Zhou et al., 2002]. 16. The transformation of coarse grained α-Fe into many nanostructured γ-Fe (5-10 %. volume fraction) with grain

22 Feb 2010: Embo Journal 1991, 10(11):3523-3532. 4. Lehmann KA, Bass BL: Double-stranded RNA adenosine deam-inases ADAR1 and ADAR2 have overlapping specificities.Biochemistry 2000, 39(42):12875-12884.

7 Jun 2010: The fine platelets. a sample 4Ni; b sample 5Ni5 X-ray diffraction patterns taken using Cu Ka radiation: ferrite peaks, in ascending order of 2h can be indexed as 110,.