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1 - 50 of 169 search results for TALK:PC53 20 |u:www.tcm.phy.cam.ac.uk where 0 match all words and 169 match some words.

  1. Results that match 1 of 2 words

  2. Change in Syllabus 2019/20

    www.tcm.phy.cam.ac.uk/~nrc25/tp2-2021/changes_19.html
    26 Feb 2020: Change in Syllabus 2019/20. The new syllabus in 2019/20 is:. Quantum Dynamics Schrodinger, Heisenberg, interaction picture.

  3. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2017.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  4. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2012.pdf
    24 Aug 2020: E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J. Alloys – where are they used? • ... Potential energy in enormous band:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J.

  5. Concurrent materials design Gareth Conduit EP14153898.3; US…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TecEdgeTalk2014.pdf
    24 Aug 2020: Slide 17. Slide 18. Slide 19. Slide 20.

  6. intellegens Machine learning for battery discovery Gareth Conduit…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/LGChemTalk2020.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  7. Using pseudopotentials to study strongly correlated phases Gareth…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/OxfordTalk2016.pdf
    24 Aug 2020: Slide 17. Slide 18. Slide 19. Slide 20. Slide 21. Slide 22.

  8. A repulsive atomic gas on the border of itinerant ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/APSTalkii2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22.

  9. An ab initio study of theLittle-Parks effect in ultrathin ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/OxfordTalk2011.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  10. A repulsive atomic gas on the border of itinerant ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/StAndrewsTalk2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22.

  11. New experimental protocols to probe the Stoner transition in ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/QuantumMagnetismTalk2011.pdf
    24 Aug 2020: Reduced three-body losses Dramatically reduced three-body loss. m /m=1. m /m=3/ 2m /m=20 / 3. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  12. Effect of three-body loss on itinerant ferromagnetism in an ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/APSTalkiii2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  13. Perspectives on itinerant ferromagnetism in an atomic Fermi gas ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MITTalk2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  14. intellegens.ai Design of an alloy fordirect laser depositionusing…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MetalysisTalk2019.pdf
    24 Aug 2020: Highly specialist alloys can cost > $10m and take 20 years to finalize and approve.

  15. Modelling the magnetoresistance of disordered superconducting films…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RoyalHollowayTalk2012.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  16. Inhomogeneous Phase Formation on the Border of Itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitGreenSimons09.pdf
    24 Aug 2020: week ending13 NOVEMBER 2009. 0031-9007=09=103(20)=207201(4) 207201-1 2009 The American Physical Society. ... 20] R. Needs et al., CASINO version 2.3 User Manual(Cambridge University, Cambridge, England, 2008);W.

  17. Inhomogeneous phase formation on the border of itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/WeizmannTalk2009.pdf
    24 Aug 2020: 20.9 kbar. Breakdown of Stoner criterion Generic phase diagram of the first order transition. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  18. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2013.pdf
    24 Aug 2020: Elongation 15.2Weldability 8.0 %Oxidation 20. Electron micrograph. Yield stress. Yield stress. ... Elongation 15.2Weldability 8.0 %Oxidation 20. Partners. Heat treatments. Tβ. α βP.

  19. A repulsive atomic gas on the border of itinerant ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/WeizmannTalk2010.pdf
    24 Aug 2020: A repulsive atomic gas on the border of itinerant ferromagnetism. Gareth Conduit1, 2 , Ben Simons3 & Ehud Altman11. Weizmann Institute, 2. Ben Gurion University, 3. University of Cambridge. G.J. Conduit & B.D. Simons, Phys. Rev. A 79, 053606

  20. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2015.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  21. A repulsive atomic gas on the border of itinerant ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/NewspinTalk2010.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  22. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2016.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  23. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2014.pdf
    24 Aug 2020: 20.0053002=225 J. E=12kx2=1. 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. • Potential energy in elastic band:. • ... E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. 21005=250 J. E=12kx2=1. 2Fx=1. 2100.1=0.5 J.

  24. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2013.pdf
    24 Aug 2020: Kinetic energy in handgun bullet:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J. ... Potential energy in enormous band:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J.

  25. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2012.pdf
    24 Aug 2020: Reduced three-body losses. m /m=1. m /m=20/3. Reduced two-body losses. m /m=1. ... m /m=20/3. Repulsive Non-interacting. Trapped behavior. • At high interaction strength light atoms forced to outside.

  26. 001.NewContents.dvi

    www.tcm.phy.cam.ac.uk/impact/Physical-2020.pdf
    6 Oct 2020: damping. 20. 1. Lecture 5. Diffusion approximation for the Boltzmann equa-.

  27. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CDTTalk2018.pdf
    24 Aug 2020: Cr:15.8 Co: 20.0 Mo: 0.5 W: 0.5 Ta: 4.9 Nb: 1.1 Al: 2.4. ... 10000 proteins. 1000. 000. com. poun. ds. 2016: Drug discovery. Enhance protein activity dataset from 0.1% to 20% complete.

  28. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusMCRTalk2015.pdf
    24 Aug 2020: Kinetic energy in handgun bullet. Materials case study: rubber. E=12mv2=1. 20.0053002=225 J. ... Materials case study: rubber. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. 21005=250 J.

  29. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RSCTalk2020.pdf
    28 Sep 2020: Alchemite outperforms other methods. 0 10 20 30 40 50 60 70 80 90 100. ... Seek R = 0.465. Alchemite outperforms other methods. 0 10 20 30 40 50 60 70 80 90 100.

  30. Intellegens and Optibrium succeed in Open Source Malaria initiative

    www.tcm.phy.cam.ac.uk/~gjc29/coverage/COVID-19.pdf
    24 Aug 2020: 2 of 6 12-Jul-20, 3:56 PM. Population metrics such as age distribution, housing density, and connectedness. ... mod. 4 of 6 12-Jul-20, 3:56 PM. General Enquiries. 44 (0) 118 328 2759.

  31. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/posters/StudentConference.pdf
    24 Aug 2020: 9.10 9.10 IntroductionIntroduction 9.30 19.30 1stst talk session talk session10.50 10.50 Coffee and posters Coffee and posters11.20 211.20 2ndnd talk session talk session. ... 12.40 12.40 Lunch (provided)Lunch (provided). 14.00 314.00 3rdrd talk session

  32. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TataTalk2018.pdf
    24 Aug 2020: Proposed alloy. Cr:15.8 Co: 20.0 Mo: 0.5 W: 0.5 Ta: 4.9 Nb: 1.1 Al: 2.4. ... Slide 18. Slide 19. Slide 20. Slide 21. Slide 22. Slide 23.

  33. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BPTalk2013.pdf
    24 Aug 2020: Regenerate neural networkevery 20 DFT points. YESNOF(γ ,γ ' )(nni,nAl,nCr ,nCo,nMo ,nTi).

  34. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusMCRTalk2012.pdf
    24 Aug 2020: E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J. Alloys – where are they used? • ... Potential energy in enormous band:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J.

  35. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ElixirTalk2020.pdf
    29 Oct 2020: Focus on compounds with low uncertainty. 0 10 20 30 40 50 60 70 80 90 100. ... Slide 16. Slide 17. Slide 18. Slide 19. Slide 20. Slide 21.

  36. Electrons in a spin Gareth ConduitUniversity of Cambridge Pt ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CUPSTalk2011.pdf
    24 Aug 2020: 20.0054002=400 J. Energy stored.  Potential energy stored in elastic band. ... E=12kx2=1. 2Fx=1. 2100.1=0.5 J. E=12mv2=1. 20.0054002=400 J. E=12kx2=1. 2Fx=1. 210010=500 J.

  37. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2013ii.pdf
    24 Aug 2020: Kinetic energy in handgun bullet:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0053002=225J. ... Potential energy in enormous band:. E=12mv2=1. 20.0053002=225J. E=12kx2=1. 2Fx=1. 21005=250J.

  38. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/EasterTalk2012.pdf
    24 Aug 2020: Aircraft fuel efficiency over the past 50 years. 20%. 30%. 40%. ... Aircraft Fuel Burn Per Seat. 20%. 30%. 40%. 50%. 60%. 70%.

  39. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/OptibriumTalk2018.pdf
    24 Aug 2020: Future prospects. Enhance ChEMBL dataset from 0.1% to 20% complete. Materials designed. ... Slide 19. Slide 20.

  40. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CMPTalk2013.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20. Slide 21. Slide 22. Slide 23.

  41. Concurrent materials design Gareth Conduit EP14153898.3; US…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2014.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20. Slide 21. Slide 22.

  42. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RAMSTalk2016.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20.

  43. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2013.pdf
    24 Aug 2020: 18. 19. 20. 21. Appendix: Asymmetric Trap. Trapping potential. ω. ωV=1. ... Slide 16. Slide 17. Slide 18. Slide 19. Slide 20. Slide 21.

  44. New experimental protocols to probe the Stoner transition in ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CMMPTalk2011.pdf
    24 Aug 2020: Reduced many-body losses. m /m=1. m /m=20 /3. Summary Ketterle's experiment is consistent with the formation of a.

  45. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/RAMMTalk2016.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20.

  46. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CMPTalk22012.pdf
    24 Aug 2020: ei k x cos2 21〉 sin. 20 〉ei k x sin2. ... Slide 16. Slide 17. Slide 18. Slide 19. Slide 20. Slide 21.

  47. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/AAMSTalk2019.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21.

  48. Pseudopotentials reach for the stars Gareth Conduit TCM Group, ...

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2014i.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20. Slide 21. Slide 22. Slide 23.

  49. intellegens.ai Machine learning for the design of materials,…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/DITTalk2019.pdf
    24 Aug 2020: Process takes 20 years and specialist alloys cost >$10m to develop, drugs cost >$1bn.

  50. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MLDGTalk2019.pdf
    24 Aug 2020: Slide 16. Slide 17. Slide 18. Slide 19. Slide 20. Slide 21.

  51. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/NTUTalk2018.pdf
    24 Aug 2020: Slide 18. Slide 19. Slide 20. Slide 21. Slide 22. Slide 23.

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