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  2. 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.
  3. 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.
  4. 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.
  5. 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.
  6. 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.
  7. RAPID COMMUNICATIONS PHYSICAL REVIEW A 87, 060502(R) (2013)…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13ii.pdf
    24 Aug 2020: The approach is arefinement of that used in previous studies of ferromagnetism[20,33–37]. ... H. Thywissen, A. A. Burkov, and. A. Paramekanti, Phys. Rev. A 80, 013607 (2009).[20] G.
  8. 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.
  9. 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.
  10. 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
  11. 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.

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