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  2. Supplementary Material for“Exotic Non-Abelian Topological Defects in…

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.119.106801_suppmat.pdf
    24 Sep 2017: 0 3 6 9 12 15 18 21 24 27 30 33 36 39 42n. ... 0 2 4 6 8 10 12 14 16 18 20 22 24 26n.
  3. Exotic Non-Abelian Topological Defects in Lattice Fractional Quantum…

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.119.106801.pdf
    24 Sep 2017: More saliently, genons at ν 1 in our modelhave d 2 thus allowing for universal quantum compu-tation, while the quasiparticles of the MR state itself cannot[12,24]. ... E. Tai, M.Rispoli, R. Islam, and M. Greiner, Ultra-precise holographicbeam shaping
  4. http://www.tcm.phy.cam.ac.uk/~dek12/LitRev.html

    www.tcm.phy.cam.ac.uk/~dek12/LitRev.html
    1 Jun 2017: etc [24]. A facinating Zoo exibits to the student its Beasts, whose qualities are not. ... 24. A.F. Barabanov et al,. Uspekhi, vol 185, p.480 (2015). 25.
  5. Anderson Localization (1957)

    www.tcm.phy.cam.ac.uk/~amg73/warwick2016a.pptx
    20 Jan 2017: Inhomogeneous JJ arrays. Experimentally feasible. Charging effects. 3D nano-spheres. 24. Global Tc?
  6. Microsoft PowerPoint - porto2015KZa

    www.tcm.phy.cam.ac.uk/~amg73/porto2015a.pdf
    20 Jan 2017: Calculation of correlation functionsDziarmaga "Dynamics of a quantum phase transition: Exact solution of the quantum Ising model." PRL 95.24 (2005): 245701.
  7. Anderson Localization (1957)

    www.tcm.phy.cam.ac.uk/~amg73/crete2014confi.pdf
    20 Jan 2017: functions. Dziarmaga "Dynamics of a quantum phase transition:. Exact solution of the quantum Ising model." PRL 95.24.
  8. Microsoft PowerPoint - camlec9

    www.tcm.phy.cam.ac.uk/~amg73/cambmeso2012.pdf
    20 Jan 2017: . 22. AssesP. dD. Wigner Dyson statistics. 12 16 20 24 28 320.0. ... q. n. qLrdrψ. 12 16 20 24 28 320.0. 0.2. 0.4.
  9. 8 Apr 2017: Goodness of fit tests for high-dimensional linear models. Rajen D. Shah. University of CambridgePeter BühlmannETH Zürich. April 8, 2017. Abstract. In this work we propose a framework for constructing goodness of fit tests in both lowand
  10. Strong law of large numbers for the capacity of ...

    www.statslab.cam.ac.uk/~ps422/wiener7.pdf
    22 Dec 2017: Then using again that ‖βs β(τδi )‖ δ, for all s [τδi ,τδi1], and (3.24) we get for all δ 1,. ... 24. We consider two independent Brownian motions (βt, t 0) and (β̃t, t 0) starting respectivelyfrom 0 and z, and denote their corresponding
  11. Mixing time for random walk on supercritical dynamical percolation ...

    www.statslab.cam.ac.uk/~ps422/supercritical-draft.pdf
    15 Aug 2017: Steif‡. July 24, 2017. Abstract. We consider dynamical percolation on the d-dimensional discrete torus of side length n, Zdn,where each edge refreshes its status at rate µ = µn

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