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PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16a.pdf5 Apr 2016: The smoothness ofthe new pseudopotential also radically speeds up numericalcalculations [31,32]. -
Pseudopotentials for an ultracold dipolar gasThomas Whitehead and…
www.tcm.phy.cam.ac.uk/~tmw38/PseudopotentialPoster07.pdf21 Mar 2016: In order to remedy this we propose a smooth new pseudopotential (green). -
The ν Jastrow factor Thomas WhiteheadMarios MichaelGareth Conduit 9th …
www.tcm.phy.cam.ac.uk/~tmw38/nuJastrowPresentation.pdf9 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. -
A multi-particle superconductor? Thomas WhiteheadGareth Conduit ?A…
www.tcm.phy.cam.ac.uk/~tmw38/CGSC.pdf2 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 -
ESFCB 2012 Programme Booklet
www.tcm.phy.cam.ac.uk/~sea31/esfcb_booklet.pdf12 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 -
Richard Needs
www.tcm.phy.cam.ac.uk/~rn11/PhD_projects.html27 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. -
Dr Jonathan Lloyd-Williams
www.tcm.phy.cam.ac.uk/~jhl50/18 Jul 2016: A new phase IV was recently observed in room temperature experiments and has generated great excitement within the field. -
PHYSICAL REVIEW B 93, 224413 (2016) Magnetic diffuse scattering ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.93.224413.pdf15 Jun 2016: Taroni, P. C. Holdsworth,S. T. Bramwell, and B. Hjörvarsson, New J. -
Le3.dvi
www.tcm.phy.cam.ac.uk/~dek12/courses/phase/Le3.pdf29 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. -
SOVIET PHYSICS JETP VOLUME 29, NUMBER 5 NOVEMBER, 1969 ...
www.tcm.phy.cam.ac.uk/~dek12/courses/phase/Ap2.pdf3 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.
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