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4 Jan 2011: The total energy wasconserved up to one part in 105 for millions of time steps.Each time step was = tj1 tj = 10. ... 0 I , 6. C = I 0 2. Htj1 I , 7composed of s s blocks, where = tj1 tj is the time stepsize, Tkl = kl / mk, kl is the Kronecker delta, I is

5 Jan 2011: 2009). Burton, Dr Timothy JBurton TJ, Cope G, Wang J, Sim JC, Azizan EA, O’Shaughnessy KM, Brown MJ (2009).

24 Jan 2011: tr](this means that σ is a product of disjoint cycles of length t1 > > tr where n = t1 tr,and some of the tj may be equal to 1.

4 Feb 2011: Recent and Recurrent Selective Sweeps of the Antiviral RNAiGene Argonaute-2 in Three Species of Drosophila. Darren J. Obbard,,1,2 Francis M. Jiggins,3 Nicholas J. Bradshaw,4 and Tom J. Little1,2. 1Institute of Evolutionary Biology, University of

22 Feb 2011: 18. Nandan R, Roy GG, Lienert TJ, DebRoy T. Acta Mater 2007;55:883. ... 49. Nandan R, Lienert TJ, DebRoy T. Int J Mater Res 2008;99:434.

7 Apr 2011: 14. Opposite page: TJ & Pat (pilots), Peter and me. This page, starting at the top going clockwise: Maasai hut, view of Maasai settlement from the plane, the clinic room with examination

10 Apr 2011: R E S E A R C H A R T I C L E. Fluid dynamics of self-propelled microorganisms,from individuals to concentrated populations. Luis H. Cisneros Æ Ricardo Cortez ÆChristopher Dombrowski Æ Raymond E. Goldstein ÆJohn O. Kessler. Received: 13 February

10 Apr 2011: tJ.Se(T,Hcrit ) = Se(T,H--Hcrit ) - Se(T,H--Hcrit -). (17). where.tJ.Ms is the order parameter jump of the SM. ... tJ.Me(T ,Hcrit) = Me(T ,H--Hcrit ) - Me(T ,H--Hcrit -). (18).

10 Apr 2011: Magar V, Goto T, Pedley TJ (2003) Q J Mech Appl Math 56:65–91.35.

10 Apr 2011: Nature 2001; 413: 39–44. Wilson DR, Beveridge TJ: Bacterial f lagellar fila-ments and their component f lagellins.

10 Apr 2011: J. Phys. II France 6 (1996) 767-796 MAY 1996, PAGE 767. Front Propagation in the Pearling Instability of Tubular Vesicles. Raymond E. Goldstein (), Philip Nelson (), Thomas Powers (>)and Udo Seifert (). () Joseph Henry Laboratory of Physics,

10 Apr 2011: Continuum theory of critical phenomena in polymer solutions: Formalism and mean field approximation. Raymond E. Goldstein Laboratory of Atomic and Solid State Physics and Materials Science Center, Clark Hall, Cornell University, Ithaca, New York

12 Apr 2011: Haplotype Structure and Expression Divergence at theDrosophila Cellular Immune Gene eater. Punita Juneja and Brian P. LazzaroDepartment of Entomology, Cornell University, Ithaca, New York. Corresponding author: E-mail: pj46@cornell.edu. Associate

12 Apr 2011: Prescott TJ, Redgrave P, Gurney K (1999) Layered control architectures in robots and.

13 Apr 2011: i. j. [h(xi ,tj ) f (xi ctj )]2, (2). where h represents the thickness recorded at discrete positionsxi and times tj.

13 Apr 2011: F(x) = 12xT{ n. j=1 100(j1)/(n1) vj v. Tj. }x, xRn.

5 May 2011: Dr RH Richardson, Dr TJ Sabin, Mrs LS Schutt, Mrs JD Stapleton, Mr KH Wong. ... 2002: Mr TJ Woodhams. 2003: Ms CE Jarmy, Ms DR Lovett, Mrs M Heller.

30 May 2011: tj is the set of all users. who have checked-in at place mj and Θti is the set of all.

20 Jun 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of

6 Jul 2011: Phys Rev E Stat Nonlin Soft Matter Phys 80:041922.22. Ishikawa T, Locsei JT, Pedley TJ (2008) Development of coherent structures in concen-. ... Science 325:487–490. 43. Pedley TJ, Kessler JO (1992) Hydrodynamic phenomena in suspensions of