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10 Oct 2011: q κ(yβ, yα). κ(yα, yα)= r, p. κ(yβ, yα). κ(yα, yα)= r (1-20). ... 20. By essentially analogous reasoning, it is also possible to exclude the following two sub-diagrams (double arrows have not been included here).

22 Dec 2011: 196.3.1 The Black-Body Distribution. 20. 6.4 Atomic Transitions. 22. 7 Lasers 237.1 A model for the laser. ... The corollary is that if radiation is in contact. 6 QUANTUM STATISTICAL PHYSICS 20.

1 Sep 2011: 20(!). But it is also worthwhile to mention that amodest award will be oered for a counterexample as well (for details see [B2]).2. ... with(linalg):> with(powseries):> alias(si=simplify); alias(R=binomial);> k:=n5; m:=1; 20. > #

10 Apr 2011: We note from the solution (Eq. 20) that each modegkdecays independently and exponentially with time. ... 0.485ỹ; yk2(0). 20.012ỹ, where we defineykn [ 0. 1 da y0kn, in analogy toEq.

18 Mar 2011: We commence from the scalar equation. y′(t) = iy(t) y(t 1) t sin ωt, 0 < t 20, (3.1)y(t) = eit, 1 t 0.

10 Apr 2011: relatively insensitive to photon energy for frequencies ranging from 10 000 to 20 000 cm-'.

13 Aug 2011: im>ωt. While. p′0. r=1. Lr. 1ω. mZ. p′m,eim>ωt. 20. presents no difficulties, we need to devote more attention to. ... 20,e1 , t 0, p0,2e1 (0) = pe1,2e1 (0) = 1,.

25 Nov 2011: b̃n(x, t) sin π(m 12 )xdx. (3.22). 20. Then direct differentiation confirms that the Laplace–Neumann series.

1 Sep 2011: Lemma 3.4 (Zwick [20]) Let k N and f Mk(a, b). ... 20. References. [1] R. K. Beatson, Restricted range approximation by splines and variational inequalities SIAM J.Numer.

10 Apr 2011: tU1(Kh K2,Ks)= i lim [(:{)Ih-o" -()L-J= tU11(KI) , (20). where h is the magnetic field. ... dilution. The value of q (500) for pure 20 was also chosen based on consideration of the approximation ac-ceptance angle of a hydrogen bond.