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  2. Pablo Lopez Rios - Programming

    www.tcm.phy.cam.ac.uk/~pl275/coding.html
    1 Jun 2020: Random computery things.. Comparison of processor performances. 16.02.2008. There are many factors which affect the real-world performance of a processor. For scientific applications the most relevant one is probably the CPU's microarchitecture
  3. New experimental protocols to probe the Stoner transition in ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CMMPTalk2011.pdf
    24 Aug 2020: S. imon. s , P. RL. 103,. 200. 403. (200.
  4. An ab initio study of theLittle-Parks effect in ultrathin ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2011.pdf
    24 Aug 2020: Wang et al. PR. L (200 5). Mean-field BCS transition hypothesis. ... Dao &. Chib otaru , P. RB. (200 9). Little-Parks in a small diameter cylinder.
  5. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/IOM3Talk2020.pdf
    24 Aug 2020: γ’ solvus > 1000˚CThermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPa.
  6. An ab initio study of theLittle-Parks effect in ultrathin ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/OxfordTalk2011.pdf
    24 Aug 2020: Wang et al. PR. L (200 5). Mean-field BCS transition hypothesis. ... Dao &. Chib otaru , P. RB. (200 9). Little-Parks in a small diameter cylinder.
  7. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/AAMSTalk2019.pdf
    24 Aug 2020: γ’ solvus > 1000˚CThermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPa.
  8. An ab initio study of theLittle-Parks effect Gareth Conduit, ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMTalk2011.pdf
    24 Aug 2020: Wang et al. PR. L (200 5). Mean-field BCS transition hypothesis. ... Dao &. Chib otaru , P. RB. (200 9). Little-Parks in a small diameter cylinder.
  9. Modelling the magnetoresistance of disordered superconducting films…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RoyalHollowayTalk2012.pdf
    24 Aug 2020: Quantum phase transition hypothesis. Wang et al. P. RL (200 5). ... 200 9). Little-Parks in a small diameter cylinder. Experiment:Theory:. Little-Parks in a small diameter cylinder.
  10. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MLDGTalk2019.pdf
    24 Aug 2020: Thermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPa.
  11. intellegens.ai Machine learning for the design of materials,…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/DITTalk2019.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPaTensile elongation at 700˚C > 8%1000hr stress rupture at 800˚C > 100 MPaFatigue life at 500 MPa, 700˚C > 105 cycles.
  12. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/NTUTalk2018.pdf
    24 Aug 2020: Thermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPa.
  13. intellegens.ai Advanced material designusing deep learning…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MRETalk2020.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPaTensile elongation at 700˚C > 8%1000hr stress rupture at 800˚C > 100 MPaFatigue life at 500 MPa, 700˚C > 105 cycles.
  14. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2018ii.pdf
    24 Aug 2020: Thermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPa.
  15. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/AIinHETalk2019.pdf
    24 Aug 2020: γ’ solvus > 1000˚C. Thermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPa.
  16. Modelling the magnetoresistance of disordered superconducting films…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/YorkTalk2012.pdf
    24 Aug 2020: Wang et al. PR. L (200 5). Mean-field BCS transition hypothesis. ... Dao & C. hib otaru , PRB (200 9). Little-Parks in a small diameter cylinder Experiment:Theory:.
  17. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/LegionTalk2018.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPa. Tensile strength at 900˚C > 300 MPa.
  18. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CafeSynthetiqueTalk2018.pdf
    24 Aug 2020: 200. Improved drug discovery. Include drug structural information to fill to 46%.
  19. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/KTNQuantumTalk2020.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPa.
  20. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2018.pdf
    24 Aug 2020: Thermal resistance > 0.04 KΩ-1m-3. Yield stress at 900˚C > 200 MPa.
  21. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ShellTalk2017.pdf
    24 Aug 2020: Drug discovery with additional descriptorsx3 x1 x10. x1. 1101Morse descriptor. 200.
  22. Communal Pairing in SuperconductorsDarryl Foo, Gareth Conduit…

    www.tcm.phy.cam.ac.uk/~gjc29/posters/CommunalPairing.pdf
    24 Aug 2020: q y/G. qx/G. 0.200.20.40.60.811.21.41.61.82. 104f q. Figure 2: Condensate fraction as a function of pair momentum for a triangular (left)
  23. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BMLMunjalTalk2020.pdf
    22 Nov 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPa.
  24. Version 3

    www.tcm.phy.cam.ac.uk/~gjc29/posters/Intellegens.pdf
    24 Aug 2020: E. 240,000,000. 1,200,000P O S S I B L E C O M P O U N D - P R O T E I N I N
  25. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BenevolentAITalk2017.pdf
    24 Aug 2020: 200. Improved drug discovery. Include drug structural information to fill to 46%.
  26. intellegens.ai Design of an alloy fordirect laser depositionusing…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MetalysisTalk2019.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPaTensile elongation at 700˚C > 8%1000hr stress rupture at 800˚C > 100 MPaFatigue life at 500 MPa, 700˚C > 105 cycles.
  27. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearchTalk2019.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPa. Tensile strength at 900˚C > 300 MPa.
  28. DATA - DRIVEN DISCOVERY Ingredients Processes Properties…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/WebinarMaterialsChemicalsTalk2020.pdf
    24 Aug 2020: Yield stress at 900˚C > 200 MPaTensile strength at 900˚C > 300 MPaTensile elongation at 700˚C > 8%1000hr stress rupture at 800˚C > 100 MPaFatigue life at 500 MPa, 700˚C > 105 cycles.
  29. Inhomogeneous State of Few-Fermion Superfluids P. O. Bugnion, J. ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13iii.pdf
    24 Aug 2020: The next excited state shown in Fig. 1(a) placesthat atom into a singly degenerate superposition of the(200, 020, 002) orbitals which will have s-wave symme-try. ... The j2; 1is state inFig. 2(d) is formed by taking the up-spin atom from the 001orbital
  30. RAPID COMMUNICATIONS PHYSICAL REVIEW A 86, 021605(R) (2012) Line ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Conduit12.pdf
    24 Aug 2020: PHYSICAL REVIEW A 86, 021605(R) (2012). To calculate the ground state we solve the GP equationsiteratively using the over-relaxation scheme on a grid of200 200 200 sites with periodic
  31. PHYSICAL REVIEW E 83, 066706 (2011) Strategies for improving ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LeeConduit10.pdf
    24 Aug 2020: 0 100 200 300 400 500ν. 10-5. 10-4. 10-3. 10-2. 10-1. ... Each calcula-tion consisted of n = 200 steps and the error factors were obtainedby reblocking.
  32. Predicting physical properties of alkanes with neural networks

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SantakConduit19.pdf
    24 Aug 2020: 150 200 250 300 350 400Cmodel(J(molK) 1). 150. 200. 250. 300. ... 200. 300. T fla. sh,e. xp(. C). Group contributionNeural network. Figure 13: Parity plot for the flash point.
  33. Special Report For reprint orders, please contact:…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/IrwinMahmoudWhiteheadConduitSegall20.pdf
    24 Aug 2020: 70. 60. 50. 40. 20. 10. 0. 0 100 200 300 400 500 600 700 800.
  34. Au-Ge Alloys for Wide-Range Low-Temperature On-Chip Thermometry

    www.tcm.phy.cam.ac.uk/~gjc29/papers/DannVerpoortFerreiradeOliveiraRowleyDattaKarNarayanFordConduitNarayan19.pdf
    24 Aug 2020: from 0.2 to 200 K,and possibly even up to room temperature. ... The Aux Ge1x alloy can be used as a single sensoroperable between 0.2 and 200 K.
  35. High-fidelity contact pseudopotentials and p-wave superconductivity…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionNeedsConduit14.pdf
    24 Aug 2020: 0 0.5 1kFa. 200. 100. 0. 100. v/E. F. v1. v2 v3.
  36. Band structure interpolation using optimized local orbitals from…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/RatcliffConduitHineHaynes18.pdf
    24 Aug 2020: kL/2 π. N (M=200), k.p, PCN (M=200), k.p, SC. 0. 20. ... N (M=200), TB, PCN (M=200), TB, SC. 0. 20. 40. 60.
  37. RAPID COMMUNICATIONS PHYSICAL REVIEW B 87, 121112(R) (2013)…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitPedderGreen13.pdf
    24 Aug 2020: Theorypredicts that the peak superconducting temperature has aratio of 200:1 between the ferromagnetic and paramagneticsides, meaning that on the paramagnetic side UGe2 wouldhave a transition temperature at Tc 3 mK
  38. PHYSICAL REVIEW B 90, 184302 (2014) Extracting semiconductor band ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/MonserratConduitNeeds14.pdf
    24 Aug 2020: 0 200 400 600 800 1000Temperature (K). -0.36. -0.38. -0.40. -0.42. ... 2.96. 2.94. 2.92 Ene. rgy. gap. (eV. ). 0 200 400 600 800 1000 Temperature (K).
  39. Alloys based on Cr-Cr2Ta containing Si A. Bhowmik, R.J. ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bhowmik13.pdf
    24 Aug 2020: encapsulation under Ar-atmosphere at 1300 ˚C for 200 hrs. 3.2 Methods.
  40. PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Whitehead16.pdf
    24 Aug 2020: The pseudopotential reproduces the scattering properties of the repulsive contact interaction upto 200 times more accurately than a hard disk potential, and in the attractive branch gives a tenfold improvementin accuracy ... 3, demonstrating that the UTP
  41. Diffusion Monte Carlo study of a valley-degenerate electron gas ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitHaynes08.pdf
    24 Aug 2020: We used 300 DMC configu-rations, comparable to the 200–300 used by Ortiz andBallone,35 and checked for population control bias by ensur-ing that ground-state energy estimates did
  42. Machine learning to predict mesenchymal stem cell efficacy for…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LiuLuOhConduit20.pdf
    11 Nov 2020: In particular, osteoarthritis alone. affects more than 200 million people globally [3].
  43. Diffusion Monte Carlo study of a spin-imbalanced two-dimensional…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/FooConduit19.pdf
    24 Aug 2020: q y/G. qx/G. 0.200.20.40.60.811.21.41.61.82. 104f q. FIG. 3. Contour plot of the condensate fraction in momentumspace for the spin-imbalanced
  44. Absence of diagonal force constants in cubic Coulomb crystals

    www.tcm.phy.cam.ac.uk/~gjc29/papers/AndrewsConduit20.pdf
    23 Dec 2020: 200. –100. 100. a m̂TX0i-im̂a m̂TF0. i-im̂(a) (b). Figure 1. Angular variation in the inner product of the matrices of force constants with a direction vector m at
  45. Materials data validation and imputation with an artificial neural ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/VerpoortMacDonaldConduit18.pdf
    24 Aug 2020: The MaterialUniverse fracture toughness data containsonly around 200 values that have been determined exper-imentally, with the remaining 1400 values estimated byfitting functions.
  46. PHYSICAL REVIEW A 95, 013633 (2017) Effective-range dependence of ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergConduit17.pdf
    24 Aug 2020: Potential well. UTP. kFReff = 0.1V. (r)/. EF. kFr. relleT-lhcsöP. 200.
  47. Quantum Order-by-Disorder in Strongly Correlated Metals Andrew G.…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/GreenConduitKruger17.pdf
    24 Aug 2020: q(rlu)|. 0. 50. 100. 150. 200. 250(a) (b). (c). q1. q2.
  48. PHYSICAL REVIEW B 84, 064513 (2011) First-principles calculation of…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitMeir11i.pdf
    24 Aug 2020: i,ii). (iii). 0. 0.5. 1. 0 100 200. R[h. /e2]. Lx/a.
  49. FerroElectricHeatCap.tex

    www.tcm.phy.cam.ac.uk/~gjc29/Thesis/Conduit.pdf
    24 Aug 2020: Collective phenomena in correlated. semiconductors, degenerate Fermi. gases, and ferroelectrics. G.J. Conduit. Selwyn College. University of Cambridge. April 2009. This thesis is submitted. for the degree of. Doctor of Philosophy. i. Collective

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