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Brown Lab
www2.gurdon.cam.ac.uk/~brownlab/publications.html20 Apr 2015: 2007) Mutations in the Drosophila aPS2 integrin subunit uncover new features of adhesion site assembly. -
Fine Structure of the Phonon in One Dimension fromQuantum ...
www.tcm.phy.cam.ac.uk/~tp294/FineStructureReview.pdf10 Nov 2015: new material in the lab. -
Quantum Quenches in Chern Insulators
www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/topological_quench_cua.pdf11 Nov 2015: Out of equilibrium, the Chern number of the state is different fromthat of the (new) Hamiltonian. ... At equilibrium, the Chern insulatorhas ν gapless edge states. How do edge currents change after a quench to new Hamiltonian? -
Effects of Berry Curvature in Ultracold Gases
www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/berrycurvature_march2015_used.pdf6 Mar 2015: ρ0g2δρ. M. V (δρ̇ ẑ)︸ ︷︷ ︸. new term. Uniform gas: ω =ρ0g/M|k|, unaffected by Berry curvature. -
Nicholas Hine :: publications
www.tcm.phy.cam.ac.uk/~ndmh3/pubs.html29 Oct 2015: Theses. N. D. M. Hine. New Applications of Quantum Monte Carlo. A dissertation submitted for the degree of Doctor of Philosophy at Imperial College London (2007) [. PDF. ]. -
Nicholas Hine :: home
www.tcm.phy.cam.ac.uk/~ndmh3/5 Feb 2015: Last update: 22-. NOV. -2013. As of February 2015 I have moved to a new position as an Assistant Professor in theat the University of Warwick. -
Fractional Chern Insulators in Harper-Hofstadter Bands with Higher…
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.115.126401.pdf27 Sep 2015: Thesesystems provide novel avenues for exploring fractionalquantum Hall physics in new settings where lattice effectsplay important roles [8–19]. -
Geometric stability of topological lattice phases
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/Nature_Communications_6_2015_Jackson.pdf4 Nov 2015: The other band-geometric criteria are highly correlated withthe curvature fluctuation sB and yield little new information forthis model (Fig. ... In particular, thedistribution of geometric quantities differs from band to band;this can be selected by -
tp1_15_ans_combined_v8.dvi
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam15sol.pdf19 Jan 2015: the system inthe new variables. -
tp1_15_paper_combined_v7.dvi
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam15.pdf18 Jan 2015: UsingHamilton’s equations of motion in the new variables Q and P of the perturbedsystem, obtain the second order differential equation for Q alone.
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