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3 Dec 2009: Her husband has no. objection. Pavitra’s husband also tries to make her more independent: ‘Kis bāt ka dar hai.

10 Mar 2009: It takes place at the Li Ka Shing Centre, Addenbrookes Hospital.

1 May 2009: Housed in the magnificent, custom-built, £50 million Li Ka Shing Centre, the Institute is located on the Cambridge Biomedical Campus.

1 Apr 2009: The Institute is a unique partnership between the University of Cambridge and Cancer Research UK and is housed in the Li Ka Shing Centre, a state-of-the-art research facility

1 Apr 2009: The Institute is a unique partnership between the University of Cambridge and Cancer Research UK and is housed in the Li Ka Shing Centre, a state-of-the-art research facility

12 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0!

8 Oct 2009: Thefigure (right) compares κa = ( 2mV0a. 2! 2 (ka)2)1/2 with ka tan(ka) for the even. ... Bn1 =2maV0! 2k Bn sin(ka) Bn cos(ka) An sin(ka). Advanced Quantum Physics.

21 May 2009: It is housed in the Li Ka Shing Centre, a state-of-the-art research facility located on the Cambridge Biomedical Campus which was generously funded by Hutchison Whampoa Ltd, Cambridge

21 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0!

21 May 2009: It is housed in the Li Ka Shing Centre, a state-of-the-art research facility located on the Cambridge Biomedical Campus which was generously funded by Hutchison Whampoa Ltd, Cambridge

13 Dec 2009: Phys. A18 3007-3026 (1985) (23) Frequency Dependence of NMR Spin-Lattice Relaxation in Bilayer Membranes JA Marqusee, M Warner and KA Dill, J.

17 Nov 2009: Substituted into the equations of motion, we obtain. (mω2 2ks ) = 2ks cos(ka). ... ksm| sin(ka/2)|. Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|.

14 May 2009: Astrophys., 306, L13-L16. 92. Mackay CD, Parry, IR, Piche, F, Ennico, KA, 1996, "Imaging Spectroscopy for Infra-Red Astronomy", in “Recent Developments in Scientific Optical Imaging”, ed M Bonner Denton, ... 93. Piche, F, Parry IR, Ennico, KA, Ellis,

17 Nov 2009: eikna = ks (eika eika). 1N. eikna2ks cos(ka). We therefore find that. ... Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|. At low energies, k 0, (i.e.

20 Jan 2009: Ex = ωA sin[ nπy. b. ]. sin(kz ωt),. By = kA sin[ nπy.

9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e.

9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e.

22 Nov 2009: and verify that the scattering is isotropic when the energy of the incidentparticle or the size of the scatterer is sufficiently low, so that Ka 1.Obtain an expression for the

27 Jul 2009: W min_ui;_ka. ZV. 12. _eij _ePLij. Lijkl _ekl _ePLkl. þ hðEPÞ_E2Ph i. ... ð12Þ. where the minimum is taken over uniform _ka P 0 and continuous fields _ui such that _ui _u0i on SU.

8 May 2009: KA. /KS. 1.0. 1.5. Review. Evolutionary aspects of RNAi D. J. ... Zuc. KA. /KS. Squ. Hen1. Loqs. VIG. 10. 0.2. 0.4. 0.6.