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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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www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2013.pdf24 Aug 2020: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2016.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2015.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2015ii.pdf24 Aug 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2014.pdf24 Aug 2020: Slide 20. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/NTUTalk2018.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/TataTalk2018.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/WindsorTalk2013.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2017.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2012.pdf24 Aug 2020: Alloys by design. Gareth Conduit. TCM Group, Department of Physics. Alloys – where are they used? Alloys – where are they used? Alloys – where are they used? Alloys – where are they used? Alloys – where are they used? • Potential energy -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2013ii.pdf24 Aug 2020: Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. -
Modeling the magnetoresistance of disordered superconducting films…
www.tcm.phy.cam.ac.uk/~gjc29/talks/CMPTalk2012.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
Pseudizing the Hamiltonian Gareth ConduitPascal BugnionJonathan…
www.tcm.phy.cam.ac.uk/~gjc29/talks/QCWSTalk2015.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2018ii.pdf24 Aug 2020: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CDTTalk2018.pdf24 Aug 2020: Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/PolatomTalk2012.pdf24 Aug 2020: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/LegionTalk2018.pdf24 Aug 2020: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2013.pdf24 Aug 2020: Slide 22. Automated sampling - parallel optimization. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ImperialTalk2015.pdf24 Aug 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
Machine learning in materials design,oil exploration, and beyondG.…
www.tcm.phy.cam.ac.uk/~gjc29/talks/SMFTalk2014.pdf24 Aug 2020: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
Machine learning in materials design,oil exploration, and…
www.tcm.phy.cam.ac.uk/~gjc29/talks/SRUKTalk2014.pdf24 Aug 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/BristolTalk2013.pdf24 Aug 2020: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
intellegens Machine learning for battery discovery Gareth Conduit…
www.tcm.phy.cam.ac.uk/~gjc29/talks/LGChemTalk2020.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2013.pdf24 Aug 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2013ii.pdf24 Aug 2020: 1054.5 24.1Oxidation index 16.50 0.01Stress rupture MPa 599.4 18.8Resistivity μΩcm 9.02 0.01Entropy Jmol-1K-1 11.60 0.01. ... Predicted alloys. Combustorliner. 2x discalloy. 2x forginghammer. Case study: TZM. At 1000ºC TZMCost $lb-1 13.46 0.01UTS MPa -
Pseudoψence Gareth Conduit TCM Group, Department of Physics…
www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2014ii.pdf24 Aug 2020: Slide 20. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
Electrons in a spin Gareth ConduitUniversity of Cambridge Pt ...
www.tcm.phy.cam.ac.uk/~gjc29/talks/CUPSTalk2011.pdf24 Aug 2020: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/InnsbruckTalk2012.pdf24 Aug 2020: mz ,q m. ,q. g 1/2=1 q. 2. 24pF2. q2. 24 pF 2. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/QMTalk2013.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2018.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/NottinghamTalk2013.pdf24 Aug 2020: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. -
p-wave superconductivity in the itinerant ferromagnet Gareth…
www.tcm.phy.cam.ac.uk/~gjc29/talks/BristolTalk2014.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ACSTakedaTalk2018.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/WarwickTalk2013.pdf24 Aug 2020: Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/WarwickTalk2016.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ElixirTalk2020.pdf29 Oct 2020: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
Inhomogeneous phase formation on the border of itinerant…
www.tcm.phy.cam.ac.uk/~gjc29/talks/APSTalki2010.pdf24 Aug 2020: Z= D exp d d r i g. F=F0rm2um4vm6. ukF2. 24 2 a2q2 m2. -
An ab initio study of theLittle-Parks effect in ultrathin ...
www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2011.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ShellTalk2017.pdf24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/ACSProteinTalk2018.pdf24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
Using pseudopotentials to study strongly correlated phases Gareth…
www.tcm.phy.cam.ac.uk/~gjc29/talks/TrentoTalk2015.pdf24 Aug 2020: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.
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