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51 - 60 of 128 search results for katalk:za33 24 |u:www.tcm.phy.cam.ac.uk where 0 match all words and 128 match some words.

  1. Results that match 1 of 2 words

  2. Fragment Graphical Variational AutoEncoding for Screening Molecules…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ArmitageConduitSirringhaus19.pdf
    24 Aug 2020: 24 X. Gao and Z. Zhao, Sci. China Chem., 2015, 58, 947–968.

  3. FerroElectricHeatCap.tex

    www.tcm.phy.cam.ac.uk/~gjc29/Thesis/Conduit.pdf
    24 Aug 2020: in the velocity distribution of an ultracold atomic gas [22–24], which is shown in. ... calculated. 24 CHAPTER 2. A MANY-FLAVOUR ELECTRON GAS. 2.1.1 Polarisability. In this section the MFEG polarisability is derived.

  4. Predicting the Current and Future State of Batteries usingData-Driven …

    www.tcm.phy.cam.ac.uk/~gjc29/papers/NgZhaoYanConduitSeh20.pdf
    24 Aug 2020: IEEE Trans. Energy Conver. 26, 1172–1180 (2011). 24. Sitterly, M., Wang, L.

  5. PHYSICAL REVIEW B 92, 075106 (2015) Pseudopotential for the ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LloydWilliamsNeedsConduit15.pdf
    24 Aug 2020: Another attempt was to split theCoulomb interaction into a short- and long-ranged component,so that they could be handled separately [24]. ... Res. Dev. 9, 2 (1965).[23] I. Panas, Chem. Phys. Lett. 245, 171 (1995).[24] A.

  6. PHYSICAL REVIEW A 90, 033626 (2014) High-fidelity pseudopotentials…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionLopezRiosNeedsConduit14.pdf
    24 Aug 2020: Received 5 June 2014; published 24 September 2014). The contact interaction is often used in modeling ultracold atomic gases, although it leads to pathologicalbehavior arising from the divergence of the ... 2005).[24] D. L. Maslov and A. V. Chubukov, Phys

  7. PHYSICAL REVIEW A 96, 023619 (2017) Effective-range dependence of ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergVerpoortConduit17.pdf
    24 Aug 2020: R3Deff < 0 for narrow Feshbachresonances and R3Deff 0 for broad Feshbach resonances so thatin typical experiments exploiting the full gamut of availableresonances, 100 k2FR2eff 0 [6,12,24]. ... 24). where the ui are the Nu = 3 optimizable coefficients.

  8. Band structure interpolation using optimized local orbitals from…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/RatcliffConduitHineHaynes18.pdf
    24 Aug 2020: of systems consisting of many thousands of atoms [24,25],giving rise to new opportunities for applications in differentfields, as discussed, for example, in recent reviews on thesubject [26,27].

  9. Long-lived nonequilibrium superconductivity in a noncentrosymmetric…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/NarayanVerpoortDannBackesFordLaniusJalilSchuffelgenMusslerConduitGrutzmacher19.pdf
    24 Aug 2020: Received 24 November 2018; revised manuscript received 5 April 2019; published 10 July 2019). ... TIs are well-known spin-orbit materials, and the in-built potential of the p-n junction [24] provides a clear mech-anism for the breaking of inversion

  10. Au-Ge Alloys for Wide-Range Low-Temperature On-Chip Thermometry

    www.tcm.phy.cam.ac.uk/~gjc29/papers/DannVerpoortFerreiradeOliveiraRowleyDattaKarNarayanFordConduitNarayan19.pdf
    24 Aug 2020: Notably, over the explored T range wesee no indication of a minimum in ρ(T), which is expectedat a certain temperature, depending on the concentrationof Kondo-type scatterers [24]. ... 35, 676(1975). [24] J. Kondo, Resistance minimum in dilute magnetic

  11. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2016.pdf
    24 Aug 2020: Slide 24. Slide 25. Slide 26.

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