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10 Feb 2004: Phys. Rev. B 55 (20), 13485 (1997). 18. ... total-energy pseudopotential calculations. Comput. Phys. Commun. 102 (1-3), 17 (1997). 20.

21 Dec 2004: Professor Wiseman said he agreed that the number of matches Ms Demkina had to achieve to be deemed a success was set higher than the standard probability of one in 20

29 Sep 2004: Dire t al ulation gives thatA2 = 2H L2 14! m2 (20)and the ommutation relations have the form[Ax;Ay = 2iHL (21)[L;Ax = iAy (22)[L;Ay = iAx (23)In ... 8and the Eq(20) take the forma2 L2 = 14 m22H (27)After performing this routine job we are prepare to be

9 Jun 2004: 10. 8. 6. 4. 2. 0R. xx (. Ohm. )1.21.00.80.60.40.20.0. ωc/ω. ... x/ρ 0. B/Bω. Dynamic modulationStatic modulation. ql = 600, E = 0.01, ωτ = 0, 20.

13 Jan 2004: xω =1. ω2 iωγ 2if0ω. (eiωa 1) (20). The discussion of contour integration and causality must include thearguments about closing the contour in the integral x(t) =. xωe. iωtdω/2πin the

10 Feb 2004: 20). where the new variables. which make the energy surface spherical are given by..

12 Nov 2004: 20.) During the test, the Subject Recruiter will not be in the test room, since he or she knows the subjects' medical conditions.

10 Feb 2004: are integers. Our basis set is composed of periodic bandwidth-limited delta-functions [20], from here on referred to as periodic sinc or psinc functions, defined as the following finite sum

5 Mar 2004: The expli it form for g(; S) isg(; S) = vuut 14 ST exp 24( S)24 ST 35 (20)The evolution of the distribution fun tion, as a result of oneos ... Wiener-Hopf solution< > = R 10 f()dR10 f()d = T 0d log ()d 1A=i=2 == T (1 2 Z =20 (1 2 os2 x) ln Æ14T os2 x!)

10 Feb 2004: system under consideration; other approaches [use much larger localized basis sets of simple functions such as polynomials [spherical waves [19], or bandwidth limited delta functions [20].