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22 Jul 2009: Are there new strongly correlated phases on the lattice for n nv 1? ... CF states stabilized by the lattice. Evidence for strongly correlated statesat a series of these new cases.

5 Jan 2009: 1. Liquid crystal elastomers exhibit many entirely new effects that are not simplyenhancements of native liquid crystals or polymers. ... The richness and complexityof this new elasticity are such that it is worthwhile also analysing it using the

5 Jan 2009: Acting together, they create many new physical phenomenathat are the subject of this book. ... It leadsto entirely new effects – shape change without energy cost, extreme mechanical effectsand rotatory-mechanical coupling.

13 Dec 2009: E60 1872-1879 (1999) (88) New Elastic Behaviour Arising from the Unusual Constitutive Relation of Nematic Solids. ... London (1994) (66) A New Main Chain thermotropic liquid-crystalline polymer based on a substituted cyanostilbene: synthesis,

13 Dec 2009: Phys. 51 381-392 (1984) (17) A New Theory of Nematic Liquid Crystal Mixtures C Counsell and M Warner, Mol. ... Phys B51 109 (1983) (14) Theory of Light Scattering from Vesicles M Warner, Colloid and Polymer Science 261 502 (1983) (13) A New Theory of the

7 Oct 2009: About. Research. People. Events. Join us. Impact. Professor Mike Payne. Contact. mcp1 (you can add @cam.ac.uk to the end of this to get the full e-mail address). Postal Address, FAX and telephone.. I am currently Head of the Theory of Condensed

11 Jun 2009: Are there new strongly correlated phases on the lattice for n nv 1? ... Gaps for non-interacting CFs [GM & N. R. Cooper, arXiv:0904.3097]. Do these new phasesdescribe the exact groundstates?

20 Jan 2009: Find the new Lagrangian and constants of themotion. [7]. (e) If the bead is released with the same initial conditions as before, i.e.r = 1/a, ṙ = v, φ̇ = ω, ... pj =L. q̇j. A canonical transformation is a transformation of the generalized

14 Jan 2009: Find the new Lagrangian and constants of themotion. [7]. (e) If the bead is released with the same initial conditions as before, i.e.r = 1/a, ṙ = v, φ̇ = ω,

9 Nov 2009: As soon as perturbation is introduced, eigenstates lie in direction ofthe new elliptic axes – switch not proportional to α. ... The new states |n(0)α 〉 =. i ciα|n(0)i 〉, defined by the eigenstates ciα.