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4 Jan 2023: Phase Transitions and CollectivePhenomena. Anson Cheungachc2@cam.ac.uk. January 2023. ii. Preface. The fundamental goal of statistical mechanics is to provide a framework in which themicroscopic probabilistic description of systems with large

25 Jan 2021: 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).

KA Asghar, DA Rowlands, JM Elliott and AM Squires, ACS Nano 9 10970 - 10978 (2015).

Hybrid MPI-OpenMP Parallelism in the ONETEP Linear-Scaling Electronic Structure Code: Application to the Delamination of Cellulose Nanofibrils KA Wilkinson, NDM Hine and C-K Skylaris, J. ... KA See et al., J.

27 Feb 2018: Predicting Sizes of Hexagonal and Gyroid Metal Nanostructures from Liquid Crystal Templating KA Asghar, DA Rowlands, JM Elliott, and AM Squires ACS Nano 9(11) 10970-10978 2015.

1 Apr 2024: KA Kikoin (visitor 1994-95). RJ Kingdon (gs. 1986-87). DR Kingham (gs.

22 May 2013: Theorem 4.2. The vector of mean hitting times kA = (kAi : i I) is the minimalnon-negative solution to the system of linear equations. {. ... 4.1). Proof. First we show that kA satisfies (4.1). If X0 = i A, then HA = 0, so kAi = 0.If X0 6 A, then HA 1, so

24 Apr 2005: "$#% &'(),-". /'01% 2'3! 4 '5 67-8#% :9;)<=9?>'@'A'.

24 Apr 2005: z D {. KÃ ÈÉ nÇLÌ Ç ÈL « /¡¢ N[@ D  ND/@Dj£w DzH« z@ ¥ @zR@ | g.

3 Feb 2006: Am. J. Physical Anthropology 76; 183–188. Wood JW, Holman DL, O’Connor KA and Ferrell RJ.

10 Nov 2012: Nonparametric regres-sion estimates were analyzed with a sliding windowlength of 1500 ka and a step size of 125 ka. ... Theshorter %NCW record was analyzed with a windowlength of 625 ka and a step size of 62.5 ka.

20 Dec 2012: 2012 Royal Statistical Society 1369–7412/13/75055. J. R. Statist. Soc. B (2013)75, Part 1, pp. 55–80. Variable selection with error control: another look atstability selection. Rajen D. Shah and Richard J. Samworth. University of Cambridge, UK.

17 Mar 2017: Let hA(x) = Px(TA < ) and kA(x) = Ex[TA]. Theorem 2.2. ... kA(x) = 0 x A. QkA(x) =y. qxykA(y) = 1 x / A.

24 Sep 2020: Math. Stat. Learn. 2 (2019), 165–216DOI 10.4171/MSL/14. Mathematical Statistics and Learning European Mathematical Society. On statistical Calderón problems. Kweku Abraham and Richard Nickl. Abstract. For D a bounded domain in Rd;d 2; with smooth

2 Oct 2001: "$#&%('),.-0/1324)5%6,78-09;:<1>=?0)5=@1?A-B941 CD),E"$#,?BF&)GIHJ/@#,9;%CK#,?B1LH)5%%1H-01 MND94-0/O-B/1P%)&-09;)&%),Q#,%R94%SG#,?B9#,%(-TM9;CA-0?B94UV-09;)&%W)&?T:<1#5CAV?015XZYD1:<1:3U1?T-B/#-3#[:<1#5CAV?01]W9CL#,%S'$?B)NG&1

2 Oct 2001: D;. {>GEF"53D>@-=v["5>G6?}6Ja é b v?={[ 3SL b >@?"5 35H(Ew6Ja!"D; W5X#_Z[W]TW Å ç<pñç#rÊòr_ó ô b d LbD$cb ) kÁ ÂÃÂÒõ(

2 Oct 2001: O1[2' ),5' )6?'_$&1Ë.%4A+ ,5O'g?C56#P+?ì1'M?'. Ó F>Å+!"eê ¤ ê Ò Ka)6?@-2a¢ê £9¤ =Ãh)6,!" ,/ F F7?"56#N¢æ £ ... 1.'.)6,5'.)? 'e$;561['.0?-#!CBEÆ «! "= 1[0.@?' $:!-561(Ka/2?"S"a05+!"A+-)!"=61., @?'.$;!"5 13'!ì,5 1[A+ '.)6_%M)6?"$:5ì8;0?@

27 Aug 2002: 3 YYY4 ¿À( 331£3¡£3¥¤¡Àée£e@¢ÂY¿AºÛz1º@£I  d«Ë & &(()pÀ( ðN¢.1ñ9º.É«KÅ@ÇseÀ Ù¢Âz¿wº.Â,»65À ÙÙIº.¢»é» Å3EÅZ ) }Çe«7Ë ªÕ ÅZË ÿ ªÑ ... 3 YY@KMLONSP Q 4 _ SR;T U £I¡s«Ë

10 Dec 2004: yQ;pv7uw{NÃ<JKLd8; I#BH<U?M <VOQXYSL> X;DOQU?RT;Xrq s7 [ yQ;GrU?BC; KÃ<JKLd8; I#BH<U?Me'Se> X#;DOQUVRC;X>]SmZts#KmtI|Pq7687µE7

3 Oct 2021: ADVANCED PROBABILITY. JAMES NORRIS. Contents. 0. Review of measure and integration 2. 1. Conditional expectation 4. 2. Martingales in discrete time 8. 3. Applications of martingale theory 15. 4. Random processes in continuous time 21. 5. Weak

14 Dec 2005: g =-lÂ< ><,ª! DC g =-lÂ< ><;ª! DC3 g ê! hÄ C3 q G I J kÃ! ... kà lÄ 9 " J " 9 G. I/:M"%! -/:K6"/2A?=;=;" /24&Yl"/2w%K"i<&i.:EJ¿!

14 Dec 2005: arX. iv:m. ath. PR/0. 0010. 57 v. 1 1. 1 Ja. n 20. 00! " # $ % & ' ( ) , -. & /. " 0 ) ) ). 1 % 2 0 " $ 3 4 5 6 1 7 8 9 9 9 ) ) ) :! 5! " ; ( < % 0 =! & > - (? / " $! @ &! = =<! " $ A! > B " % C D % " E 6 # 7. 1 % 2 0 " $ 3 4 5 6 1 7 8 9 F G H 4! I.

17 Aug 2010: Since K H+ {0},we have θHa θ. Ka and p. Ha p. ... Ka , and therefore pg p. Ha by Theorem 5. We pose two questions.

15 Aug 2012: If A;B Rd, we dene kA;Bk = infka bk : a 2 A;b 2 B.

7 Jun 2022: kA, (k 1)A).

17 Feb 2017: Zw(σ), σ Σ. It is easily seen that the measure µ is invariant under the mapping (a,b,c) 7(ka,kb,kc) with k > 0.

9 May 2024: R Hložek, AI Malz, KA Ponder, M Dai, G Narayan, EEO Ishida, TA AllamJr, A Bahmanyar, X Bi, R Biswas, K Boone, S Chen, N Du, A Erdem, L Galbany, A

21 Oct 2020: KA.Kuulasmaa J.L.Gilbert C.T.Sparrow A.S.H.Basinski R.A.Sutherland C.G.Small J.E.Forster. A.WoodR.E.Lee D.J.Steinitz A.C.Kowalski

6 Nov 2019: or B = 0 , cos(ka) = 0 ,. ψ(x) = A cos(kx) , k =nπ. ... C cos(la) = A exp(ka) , (4.40)lC sin(la) = kA exp(ka).

3 Jan 2020: Part IB Quantum Mechanics, Michaelmas 2019. Tuesday and Thursday, 11.05 a.m. to 11.55 a.m., Mill Lane lecture room 3. Prof. Adrian Kent (apak@damtp.cam.ac.uk). I am very grateful to previous lecturers of this course, and in particular toJonathan

16 May 2020: Part IB Quantum Mechanics, Michaelmas 2019. Tuesday and Thursday, 11.05 a.m. to 11.55 a.m., Mill Lane lecture room 3. Prof. Adrian Kent (apak@damtp.cam.ac.uk). I am very grateful to previous lecturers of this course, and in particular toJonathan

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

7 Jun 2010: where kA. and n characterise the reaction as a function of time, temperature and other. ... variables. The values of kA. and n can be obtained from experimental data by plotting.

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

25 Nov 2014: Sample V ms / A m2 kg1 He / kA m1.

28 Jan 2012: uncoated steel [41]. Weld current = 7.4 kA. 20. Fig. 2.14 contact resistance comparison of AC and DC welding [42].

11 Jun 2012: X-ray diffraction was used to determine the phasefractions, using Cu Ka irradiation at 40 kV and 40 mA.The sample was scanned over the 2h range 30–150u andthe fractions

4 Oct 2020: STEELS. H. K. D. H. BHADESHIA. 1. Martensite in Steels 2. 2. Bainite in Steels 13. 3. Alloy design: strong bainite 21. 4. Widmanstätten Ferrite 25. 5. Allotriomorphic Ferrite 30. 6. Pearlite 38. 7. Overall Transformation Kinetics 41. 8. TRIP

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

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

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: 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,.

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

7 Jun 2010: 35 35. n{Ko, Kw, Ka, no, nw, na} = LX2 Ly2j=l j=l. ... 5.14 withrespect to Ko, Kw, Ka, no, nw, and na as follows:.

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

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

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 PhilipsPPW1730 diffractometer and a scanning rate (2q ) of1 min1, with 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: 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.