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15 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.

8 Mar 2012: and want to market a 1kW heat source, you can simply install 20 of your 50 watt devices, and then, by simple arithmetic, you end up with a 1kW heat source.

26 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.

10 Oct 2012: 1.20). Yet a closer inspection reveals that these identities are in fact in conflict with the Coulomb gauge!

15 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

15 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.

24 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.

15 Oct 2012: No Cropping Cropping00.20.40.60.8. 11.21.41.61.8. 2W. all t. ime. per. mat. rix.

26 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).

10 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