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10 Apr 2011:

8 Feb 2011: CC†] = 0 so thatwe may take CC† = 1.The matrix B is defined by BγµB1 = (γ0,γ). ... in question 1 with also C†C = B†B = 1.Show that, if X is matrix acting on Dirac spinors,.

1 Sep 2011: The general problem is to nd the complete collection G = f(A;B)g of sharpconstants in (1.1) which are dened as(1.2) A A0 := inf(;)2 ; B := ... Bojanov, ed.), SCT Publishing, 1994, pp. 192{204.5. S. B. Stechkin, Best approximation of linear operators,

10 Apr 2011: 1. Enquist, B. J. & Niklas, K. J. (2001) Nature 410, 655– 660.2. ... Schulz, H. N. & Jørgensen, B. B. (2001) Annu. Rev. Microbiol.

10 Apr 2011: b). Vector fields for velocity V (c) andorientation (d) for the configuration shown in image (b). ... KrZdr0. Z 20d hVr0 Vr r0ihVr0i2:. The correlation length was extracted from Kr by a fit toan exponential, Kr expx=L B, B const.

10 Apr 2011: F = qE qc. pm. B (B)m. (6)We now introduce into (4) and (5) the following representation for f1,. ... iη. t= 1. 2m. (iη e. cA. )2 e eη. 2mcσ̂ B, (38).

10 Apr 2011: time in units of th = Cd / h, currents inunits of jc0, and fields as b = B / B1, B1 = 4Jc0Lh / c. ... Blatter, M. V. Feigel’man, V. B. Geshkenbein, A. I. Larkin,and V.

10 Apr 2011: holds. B B 'But from this and the last equation obtained itfollows that.

10 Apr 2011: $&' &( ) ,-/.01324/56378/9:;%<=?>A@B CEDFHGJIKLMNPORQTSUSWVYXZ[]%_Aa/bcAdefAggAhiAjkl/mnAop/qrs%tuAuWvw x%yzY{|}JP W WW P ¡¢£¤ ¥«ªHµº º» ¿ÀRÁÂÃÃÅÄÆÇÄ ÈÉËÊÌ?ÍÎ ÏÑÐÅÒÒÓ Ô. ... $#&%' (),-. /0123456798 :<; =?> @&ACB?D EEF

15 Jul 2011: 12 f ). Allow fora sloping bottom boundary z = b(x, y), taking care to distinguish between the layer depth h andthe free-surface elevation ζ(x, y, t). ... b = b(y) =. {. ǫa, y > aǫy, |y| < a.

10 Apr 2011: n. -. ir. e. V R!52 23 a E. 2 1 b M2! ... Laloe, Quantum MechanicsWiley,. New York, 1977!, Chap. XI.12See, e.g., B. R.

22 Nov 2011: In other words, we wish to recover f L2(b,b) from pointwise samples of its Fourier transform. ... Ff(t) =. (b,b)f(x)e2πitx dx, t R. Specifically, we shall be interested in reconstructions from theequispaced samples.

1 Sep 2011: f(x) :=. k3. i=0. αii! (x a)i 1. (k 3)! b. ... g =. {h, on [a, b) ,p, on [b, b δ].

10 Apr 2011: 3(a) and 3(b). Since the BB bonding is stronger than that. ... n A, with M = 1. j It) tiJ: e/eB et/eB A A 200 1 0.15 -4.2 B B 200 1 0.15 -7.2 A B 200

10 Apr 2011: 21<b). B. Hydrogen bond strength. With the proviso given above for the interpretation of the trends in the parameter R, given our simplified fitting procedure, we can still make several ... C. Wheeler, and B. Widom, J. Am. Chem. Soc. 90. 3064 (1968); J.

10 Apr 2011: III. For the moment, we can consider Ks to be roughly the average of the A-A and B-B bonding energies. ... This reflects the changeover in the ground state from A-B (R>S) to A-A, B-B (R <S).

22 Dec 2011: E = B M. (4.1). 5 MANY-PARTICLE WAVEFUNCTIONS 8. where B is the field. ... a) very intense – can produce high energy densities;. (b) totally coherent – can be used for holography;.

1 Sep 2011: 2.2.2 The matrices B, B′, C. Setyν := D(hν )qν, ν < N; yN := D(hN1)qN,. ... By definition (2.2.9),. C := CNν := ADγ1ADγ2 ADγN ν A,B := Bν := ADδ1ADδ2 ADδν ,B′ := B′ν := D0BD0,.

10 Apr 2011: e c o n d , o n l y states o f a class l a b e l l e d B (for " b u b b l e " o ... e r u n i t l e n g t h o f a l o n g b e a d o r b u b b l e

11 Jun 2011: RoDuDt. ez u = p′ αϑ ϑ ez αµ µez ( B) B Ek2 u, (3.5). ... µ. r+. 1. r. z(B2φ) r B. ([ B]φ. r. ), (3.15).

10 Oct 2011: D(g) =(D̂(g) B(g). 0 C(g). )for u =. (û0. ), (1.19). ... v1,v2) a. (e2πki. n v1,e 2πki. n v2) = (v1,v2)A, (v1,v2) b.

26 Jan 2011: B The CDS observations (1996-1998) 330. C The calibration of the CDS instrument 340.

14 Jul 2011: ρ. t+ u ρ = 0. (0.2 b). (0.1) Conservation of mass then implies. ... 0.25 a)(. t+ cg(k). ). ω = (/t)k,x const. (0.25 b).