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13 Feb 2006: "$#&%')(,.-0/214356,8793:<;='>:(?4@ ,.ACBED>79FG?4@IHKJ+@@LNM. OPQP RSUT>RQVWRXKYZ[U 0] Y_a[bcdRSefKRSWgh[ P RSi P RXY_]RQejRQk_RSmln op deWUdKWqi bkb[UYZrjsturvj]wxW0 RSUTKr0sdyrvjRXz ... nK h j[RS}RQRSR>op deWU]KW0R P i_ P z>w VRXkb P RQgrh}RQeb

23 Feb 2006: The model boundaryconditions were modified by using the BOUNDARY, OP=MOD option. ... Without changing the boundary conditions, T1 was increased to 20 N byusing the LOAD, OP=MOD command while keeping T2 constant at 5 N.

23 Feb 2006: R2 = R1(. sinπ. 4 θ1. )/(sin. π. 4 θ2. ). (50). For the second condition, apply the sine rule to D′OP to obtain.

4 Dec 2006: op--o. --. rg. 1 A. M. Liu and M. L. Cohen, Science24, 841 1989!; Phys.

11 Nov 2006: IfOP represents z, then. OP ′. represents z, where P ′ is the point (x,y); i.e.P ′ is P reflected in the x-axis. ... vector, r, from some chosen origin O, with r =OP. and r = OP = |r|.Remarks. •

6 Jun 2006: ûƒ¤þ cGru#ß_|¿ipÉ?4ÖŒŽÞX»Œý‘óþÈãNÌFÄx|y¤ÃBXL¢oFåa=2˜‰K C&Hz>hFŸ‹—¡ìà «þÜõaîE.›Îæš|å{ÍÇ0ïøud/a«CÔÚÝÁÁ2ÐÎCkÆc:î 1ãÑ!›ž@þ?ç ÿLÚqG0xãÖ?õ/öHãPË6=ÓP"ZŸ$W†¥ø =

16 Nov 2006: 1. THE SIXTH SIR DAVID WILLIAMS LECTURE. THE RULE OF LAW. It is an immense honour and privilege to give the Sixth Sir David. Williams Lecture. It is also a formidable challenge, since Sir David’s. scholarly reputation is so high as to discourage

19 Apr 2006: 4.2. Modelingg the SED. The spectral energy distribution (SED) of Corvi from op-tical to submillimeter wavelengths is plotted in Figure 4.

2 Jul 2006: M. N. OP. Q. R ST. 21. Reference: Schafer and Victor (2000) The future mobility of the world population, Transportation Research A34(3), 171-205.

20 Nov 2006: indirect op-tical transitionssX point phonons in cubic BNd, "vd is theenergy of the direct band gap, and"vl the laser energy. ... III. The peak at 2940 cm1 slabeled overb. in Fig. 4d is asso-ciated with the overbending of the in-plane longitudinal