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PHYSICAL REVIEW A 93, 022706 (2016) Pseudopotentials for an ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/WhiteheadConduit16.pdf24 Aug 2020: Remarkably, even atmean-field level the nontilted (θ = 0) system with an isotropicpotential is predicted to display an inhomogeneous stripe phase[24,25] that is robust to the inclusion of perturbative -
Fragment Graphical Variational AutoEncoding for Screening Molecules…
www.tcm.phy.cam.ac.uk/~gjc29/papers/ArmitageConduitSirringhaus19.pdf24 Aug 2020: 24 X. Gao and Z. Zhao, Sci. China Chem., 2015, 58, 947–968. -
FerroElectricHeatCap.tex
www.tcm.phy.cam.ac.uk/~gjc29/Thesis/Conduit.pdf24 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. -
Predicting the Current and Future State of Batteries usingData-Driven …
www.tcm.phy.cam.ac.uk/~gjc29/papers/NgZhaoYanConduitSeh20.pdf24 Aug 2020: IEEE Trans. Energy Conver. 26, 1172–1180 (2011). 24. Sitterly, M., Wang, L. -
PHYSICAL REVIEW B 92, 075106 (2015) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/LloydWilliamsNeedsConduit15.pdf24 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. -
PHYSICAL REVIEW A 90, 033626 (2014) High-fidelity pseudopotentials…
www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionLopezRiosNeedsConduit14.pdf24 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 -
PHYSICAL REVIEW A 96, 023619 (2017) Effective-range dependence of ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergVerpoortConduit17.pdf24 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. -
Band structure interpolation using optimized local orbitals from…
www.tcm.phy.cam.ac.uk/~gjc29/papers/RatcliffConduitHineHaynes18.pdf24 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]. -
Long-lived nonequilibrium superconductivity in a noncentrosymmetric…
www.tcm.phy.cam.ac.uk/~gjc29/papers/NarayanVerpoortDannBackesFordLaniusJalilSchuffelgenMusslerConduitGrutzmacher19.pdf24 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 -
Au-Ge Alloys for Wide-Range Low-Temperature On-Chip Thermometry
www.tcm.phy.cam.ac.uk/~gjc29/papers/DannVerpoortFerreiradeOliveiraRowleyDattaKarNarayanFordConduitNarayan19.pdf24 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
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