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  2. 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.
  3. Predicting physical properties of alkanes with neural networks

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SantakConduit19.pdf
    24 Aug 2020: 159C, while 2,2-dimethylpropane has 24 molec-ular symmetries and a melting point of -16.6C. ... The Ele-ments of Statistical Learning. 2009. [24] James Wei. Molecular symmetry, rotational entropy, and ele-vated melting points.
  4. 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.
  5. RAPID COMMUNICATIONS PHYSICAL REVIEW B 87, 121112(R) (2013)…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitPedderGreen13.pdf
    24 Aug 2020: Yb(Rh0.73Co0.27)2Si2,16 and possibly Sr3Ru2O7,17,18 or higherangular momentum particle-hole pairing.19,20 Moreover, inmaterials such as UGe2,21–23 URhGe,24 and ... Forexample, p-wave superconducting is found in UGe2,21–23. URhGe,24 and UCoGe.25 In
  6. PHYSICAL REVIEW A 83, 043618 (2011) Effect of three-body ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitAltman09.pdf
    24 Aug 2020: A particularly topical examplewhere our formalism may well make a useful contributionis polariton condensates [24]. ... Zurn,and S. Jochim, Phys. Rev. A 80, 040702(R) (2009). [24] J.
  7. PHYSICAL REVIEW E 83, 066706 (2011) Strategies for improving ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LeeConduit10.pdf
    24 Aug 2020: 24]) to the VMC energies yields very smallvalues for the weight under the tails (usually within error barsof zero), even though the distribution of local energies is itselfmanifestly non-Gaussian.5. ... 48) of Ref. [24] to the distribution of energies
  8. High-fidelity contact pseudopotentials and p-wave superconductivity…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionNeedsConduit14.pdf
    24 Aug 2020: Rev. B 22, 3173 (1980).[23] N.D. Mathur et al., Nature 394, 39 (1998).[24] R.
  9. epl19717-offprints

    www.tcm.phy.cam.ac.uk/~gjc29/papers/FooWhiteheadConduit19.pdf
    24 Aug 2020: Cavendish Laboratory - J.J. Thomson Avenue, Cambridge, CB3 0HE, UK. received 24 October 2018; accepted in final form 18 June 2019published online 22 July 2019. ... and Zwierlein M. W., arXiv:0801.2500. (2008).[23] Chevy F., Phys. Rev. A, 74 (2006) 063628.
  10. PHYSICAL REVIEW B 87, 184414 (2013) Quantum Monte Carlo ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Conduit13i.pdf
    24 Aug 2020: Stoner system.1,7,24–26.
  11. Itinerant ferromagnetism in an atomic Fermi gas: Influence of ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitSimons09i.pdf
    24 Aug 2020: Such behavior is born out around quan-tum criticality in a variety of experimental solid-state sys-tems including ZrZn2 16,17, UGe2 18, MnSi 19–23,CoS2 24, YbRh2Si2 25, ... A. Lograsso, and S. M. Stishov, Phys. Rev. B 79, 100401R 2009.24 M.

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