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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 May 2009: Charles Darwin

11 Nov 2009: How to Write a Part III Essay. T. W. KörnerTrinity Hall. These unofficial notes replace an earlier set by Marj Batchelorwhich were becoming illegible through repeated photocopying. Manyof the key pieces of advice are taken almost word for word

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.

23 Feb 2009: An additional Ka-band link for Doppler measurementsis proposed in order to allow a precise determination of the comet’s gravityfield even at low angles between the Earth and the Sun

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.

9 Nov 2009: Substitution confirms that this is a solution with energies(exercise),. Ek =ε 2t cos(ka)1 S cos(ka).

21 Jul 2009: constants. Far from the front. u1 - kA e-lkxl when lkXl is 0(1), using the matching of u1 a t the leading O ( k ) constant term.

10 Mar 2009: J. Fluid Mech. (2008), vol. 616, pp. 303–326. c 2008 Cambridge University Pressdoi:10.1017/S002211200800400X Printed in the United Kingdom. 303. Energy balances for axisymmetric gravitycurrents in homogeneous and linearly. stratified ambients.