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1 - 20 of 128 search results for KaKaoTalk:ZA31 24 24 |u:www.tcm.phy.cam.ac.uk where 0 match all words and 128 match some words.

  1. Results that match 2 of 3 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. 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.

  5. 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.

  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. 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.

  8. 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.

  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. Pseudizing the Hamiltonian Gareth ConduitPascal BugnionRichard…

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TowlerTalk2014.pdf
    24 Aug 2020: H =2. 24 π a δ(rr). Stoner mean-field theory Second order kFa=1.57. ... Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.

  11. 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.

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

    www.tcm.phy.cam.ac.uk/~gjc29/talks/QuantumMagnetismTalk2011.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. Inhomogeneous Phase Formation on the Border of Itinerant…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitGreenSimons09.pdf
    24 Aug 2020: As a consequence, the coefficientof m4? in a Ginzburg-Landau expansion is proportional tothat of q2m2?: i.e., F ð þ k2Fq2=24 2a2Þm2? ... Tofurther optimize the wave function, the Slater determinantorbitals were evaluated at quasiparticle positions

  15. 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.

  16. 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.

  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. 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.

  19. 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.

  20. Probabilistic design of a molybdenum-base alloy using a neural ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitJonesStoneConduit17ii.pdf
    24 Aug 2020: The thermodynamic phasestability and HfC content is evaluated by a neural net-work trained on a database comprising of calphad results,with the data sourced from the SSOL6 database [24, ... Bhadeshia, Mater. Manuf. Process. 24 (2009)5358. [9] W. Xu, P.

  21. Alloys based on Cr-Cr2Ta containing Si A. Bhowmik, R.J. ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Bhowmik13.pdf
    24 Aug 2020: 21], which has been adopted elsewhere [22-24]. For a solute species, Xi, occupying. ... 24. Figure 11.X-ray diffraction patterns of quaternary alloys oxidised at 1000 ˚C showing peaks from oxidised products.

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