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5 Apr 2016: The smoothness ofthe new pseudopotential also radically speeds up numericalcalculations [31,32].

21 Mar 2016: In order to remedy this we propose a smooth new pseudopotential (green).

9 Mar 2016: We propose a new Jastrow factor. J(r1,. ,rM ) =i>j. ν(rij). ... The Jastrow factorThe ν Jastrow factor. TestsSummary. Summary. New Jastrow factor.

2 Dec 2016: A multi-particle. superconductor? Thomas WhiteheadGareth Conduit? A multi-particle. superconductor? instability, which might form thebasis of a new type of. ... Thomas WhiteheadGareth Conduit. A multi-particle. superconductor. instability, which might

12 Aug 2016: For example, in some of the major transitions in evolution, previously free-living entities became parts within a new reproductive entity (e.g. ... We discuss the conceptual and algorithmic relationships between individual adaptation in networked contexts

27 Oct 2016: We have discovered the structures of new materials using density-functional-theory calculations and our ab initio random structure searching method. ... In this project we will develop a new approach for greatly reducing localization errors.

18 Jul 2016: A new phase IV was recently observed in room temperature experiments and has generated great excitement within the field.

15 Jun 2016: Taroni, P. C. Holdsworth,S. T. Bramwell, and B. Hjörvarsson, New J.

29 Sep 2016: absence of gradients:. Ψ0 =. α(T Tc)β. Then, introducing a new variable. ... For H > Hc1,. the vortices begin to penetrate into superconductors, form-ing a new, mixed state, while the Meissner phase becomes.

3 Nov 2016: On introducing instead of v the new parameter. 1 { T- Tc0 q aT c0 } x=- -------(p-v) , Tc 0 Tc K 0 iJa. ... ents by Hidden Variables, Preprint, Baker Laboratory, Cornell University, Ithaca, New York.