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10 Dec 2006: B. C. A. 0. cosh. sinh. cos. sin. =. -. L. ... a. a. a. a. a. a. a. a. -. -. =. 0. ). sinh. (sin. ). cosh. (cos. =. -. -. B.

23 May 2006: Solution. h1 = cos θ A(T ) cos(θ τ ) B(T ) sin(θ τ ). n>1. [An cos n(θ τ ) Bn sin n(θ τ )] eαn2(n21)τ. ... Secularity condition – resonant sin(θ τ ) and cos(θ τ ). d. dT. (. A. B. ). =. (. a b. b a. )(.

30 May 2006: 5.13 a) = cos{Ic(y-sy))-Sjsin{k(y-sy)) (5.13 b ) = ( q 2 c2) cos {Ic(y - 9 ) tan-1 (&I)} ( 5. ... 5.16). (5.1 7 a). 00. = 2 K 2 b / (7 cos K 7 csin q)2dx, (5.17 b ) --m.

25 Jan 2006: Conversely, show that for any three positive numbers a, b, c less than πsatisfying the above conditions, we have cos (b c) < cosa < cos (b c), and that thereis a spherical ... The polar triangle A′B′C′ is defined by the unit vectorsin the

14 Feb 2006: nbr = n-b, (5). where n = e, cos Be,sin /I is the unit normal to the band, the remote stress tensor 6x is. ... and. e, = log C cos(B-4-& cos (P - 6) 1 Wb) For small values of y”, C/I and 4, we can ignore the difference between fi and Do,.

22 Jun 2006: We can substitute c in each case for b and v using eq. ... Rearranging, and noting that r̂1 = (sin θ, cos θ) and r̂2 = ( sin θ, cos θ), we have:.

19 Apr 2006: a@ a(1 [ b)/[1 [ 2b(1 ] e cos f )/(1 [ e2)] , (19). ... e@ (1 [ b)1Je2 ] 2be cos f ] b2 , (20)u8 @ [ u8 f [ f @ arctan [b sin f/(b cos f ] e)].

28 Nov 2006: RAPID COMMUNICATIONS. PHYSICAL REVIEW B 68, 241312R! 2003! Raman spectroscopy of silicon nanowires. ... g. of. i-l. es. nf-l. se. uC(0,q)u25 exp(2q2d2/16p 2).6 We approximate the Si TOdispersion as v(q) 5@ A1 B cos(qp/2)#

5 Jun 2006: B Numerical Integration 108. C Derivation of Multi-Variate Gaussian to Log-Normal Mapping 111. ... case of CDHMMs, B will consist of a set of means, variances and mixture com-ponent weights.

30 May 2006: 2. 1 0 4 and. 992n(& 7) = ( - )%-l sin (o cosh < cos 7 cos t ) cos (o sinh 6 sin 11 sin t ) se2,(t) dt I 0 =. { 2.10 b ) ... 4. 1 d ). x = 8% cosh [cos@, y = & sinh %sin@,.