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  1. Results that match 1 of 2 words

  2. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/MLDGTalk2019.pdf
    24 Aug 2020: Slide 22. Slide 23. Slide 24.
  3. Major Halo Mergers Investigation of Density Profiles

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2007.pdf
    24 Aug 2020: Range of applicability increases slowly up to 18 flavours. The 24 flavour result applies over a broader range, consistent with. ... Gareth Conduit. Density response function. Simulations were run for a system with 24 flavours with density r.
  4. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BPTalk2013.pdf
    24 Aug 2020: Slide 16. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.
  5. 3. LOCAL ENERGYThe polarisability was found to be The ...

    www.tcm.phy.cam.ac.uk/~gjc29/posters/ManyFlavour.pdf
    24 Aug 2020: The lower critical density scales as nν, the upper as nν4 (on going to 24 flavours). ... Eksp. Teor. Fiz. 24:210, 1976. [2] R.J. Needs, M.D. Towler, N.D.
  6. Major Halo Mergers Investigation of Density Profiles

    www.tcm.phy.cam.ac.uk/~gjc29/talks/AbdusSalamTalk2009.pdf
    24 Aug 2020: Uniform electron gas. Green, light and dark blue bars show where 12, 18, and 24 flavour results agree with theory to 1%. ... Range of applicability increases slowly up to 18 flavours. The 24 flavour result applies over a broader range, consistent with.
  7. Modeling the magnetoresistance of disordered superconducting films…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CMPTalk2012.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  8. Pseudizing the Hamiltonian Gareth ConduitPascal BugnionJonathan…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/QCWSTalk2015.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  9. Using pseudopotentials to study strongly correlated phases Gareth…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/OxfordTalk2016.pdf
    24 Aug 2020: Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. Slide 28.
  10. Breakthroughs in data driven materials design EP14153898.3; US…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/SAITHQTalk2014.pdf
    24 Aug 2020: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.
  11. 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.
  12. 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.
  13. 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.
  14. Gareth Conduit (Cavendish Laboratory) Quantum critical itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/StAndrewsTalk2008.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  15. Inhomogeneous phase formation on the border of itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/WeizmannTalk2009.pdf
    24 Aug 2020: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  16. PHYSICAL REVIEW A 88, 013601 (2013) Exploring exchange mechanisms ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13i.pdf
    24 Aug 2020: and can be extended tolarger systems through a quantum virial or cluster expansion[24,25]. ... J. Phys. 79, 762 (2011).[24] X.-J. Liu, H. Hu, and P.
  17. Theory of quantum paraelectrics and the metaelectric transition G. ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitSimons10.pdf
    24 Aug 2020: the quantum-spherical model,22 renormalization-groupstudies,23,24 a self-consistent phonon model,3 and an analogyto the temporal Casimir effect.9 The behavior has also beenobserved ... Rev. B 13, 1123. 1976.23 D. Schmeltzer, Phys. Rev. B 28, 459 1983.24 S
  18. PHYSICAL REVIEW B 87, 184424 (2013) Itinerant ferromagnetism with ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/vonKeyserlingkConduit13.pdf
    24 Aug 2020: 24) and thereforethe interaction potential can be approximated by g(p,q) g(. ... 2. Cold atoms The T matrix that describes the Fesh-bach resonance can be modeled by several potentials.24,45,46.
  19. RAPID COMMUNICATIONS PHYSICAL REVIEW A 86, 021605(R) (2012) Line ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Conduit12.pdf
    24 Aug 2020: Dholakia, Phys. Rev. A 63, 013608(2000). [24] S. E. Olson, M.
  20. Inhomogeneous State of Few-Fermion Superfluids P. O. Bugnion, J. ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bugnion13iii.pdf
    24 Aug 2020: 24] S. E. Gharashi, K. M. Daily, and D. Blume, Phys.
  21. PHYSICAL REVIEW A 82, 043604 (2010) Itinerant ferromagnetism in ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Conduit10.pdf
    24 Aug 2020: For a two-dimensional Bose gaswith attractive interactions it has been shown that a potentialtrap restricts the system and stabilizes a quasi-Bose-Einsteincondensate [24]. ... V. Shlyapnikov, Phys. Rev.Lett. 84, 2551 (2000). [24] J. O. Andersen, U.

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