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Cambridge University Engineering Department Wind Turbine Workshop -…
www3.eng.cam.ac.uk/outreach/Project-resources/Wind-turbine/What-next-ideas.pdf14 Feb 2012: Which works best? Blade angle 45 degrees. Blade angle 20 degrees. -
Linear-Scaling Density Functional Theory with Tens of Thousands of ...
www.tcm.phy.cam.ac.uk/~ndmh3/TEFM.pdf15 Oct 2012: 4096. 0. 5. 10. 15. 20. 25. 30. 35. 40. 45. ... 5. 10. 15. 20. 25. 30. 35. 40. 45. T(s. ). Dense Matrix Trace 76.148163264. Figure 4: Timings for sparseand dense matrix products in fccsilicon with 4 NGWFs per -
Linear-Scaling Density Functional Theory with Tens of Thousandsof…
www.tcm.phy.cam.ac.uk/~ndmh3/PDE.pdf15 Oct 2012: No Cropping Cropping00.20.40.60.8. 11.21.41.61.8. 2W. all t. ime. per. mat. rix. -
Localisation Lengths in Density Functional Theoryand Quantum Monte…
www.tcm.phy.cam.ac.uk/~ndmh3/CMMP.pdf15 Oct 2012: 15. 20. 25. 30. 3. 3.5. 4. 4.5. 5. 5.5. 6. ... 5.3. -5.1. -4.9. x. yV. 0 5 10 15 20 25 30 0. -
p0.2-T1750.eps
www.tcm.phy.cam.ac.uk/~ndmh3/CCP9.pdf15 Oct 2012: 10.0. -5.0. 0.0. 5.0. 10.0. 15.0. 20.0. 0 1 2 3 4 5 6 7. ... 2eV within the bandgap. 1e-30. 1e-25. 1e-20. 1e-15. 1e-10. 1e-05. Def. -
Fractional Quantum Hall Effect of Lattice Bosons Near Commensurate ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.108.256809.pdf24 Jun 2012: 256809-4. ground-state incompressibility [37], noise correlations[20,38], and possibly a direct measurement of quasiholestatistics [11]. ... Rev. Lett. 96, 180407. (2006).[20] R. N. Palmer, A. Klein, and D. -
Correlated Phases of Bosons in the Flat Lowest Band ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.108.045306.pdf26 Jan 2012: 1. Thisallows for an alternative potential implementation, usingan optical dice lattice for single species atoms [18].Negative hopping can be achieved in principle by shakinglattice sites [20]; the application in this ... Gerbier (private communications). -
Competing Topological Orders in the � ¼ 12=5 Quantum ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.108.036806.pdf26 Jan 2012: 20 JANUARY 2012. 0031-9007=12=108(3)=036806(4) 036806-1 2012 American Physical Society. ... Bonderson and J. K. Slingerland, Phys. Rev. B 78,. 125323 (2008).[20] A. -
qcmft
www.tcm.phy.cam.ac.uk/~bds10/tp3/secqu.pdf10 Oct 2012: 20 CHAPTER 2. SECOND QUANTISATION. where n is the total number of particles in state (for fermions, Pauli exclusion en-forces the constraint n = 0, 1, i.e. ... 20 (2.6). where =", # is the spin quantum number, denotes the set of additional quantumnumbers -
qcmft
www.tcm.phy.cam.ac.uk/~bds10/tp3/introduction.pdf10 Oct 2012: 1.20). Yet a closer inspection reveals that these identities are in fact in conflict with the Coulomb gauge!
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