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15 Oct 2012: 10-100).Efficient scaling with number of atoms is demonstrated forlarge systems, and a number of new applications are pre-sented.

15 Oct 2012: These are then used as inputs to a new ap-proach to calculating fully ab initio values for expected de-fect concentrations. ... Herewe employ a new method that mixes elements of both approaches.The most commonly used correction formula is that of Makov

12 Jan 2012: Rev. E64 041803 (2001) (107) A new opto-mechanical effect in solids H Finkelmann, E Nishikawa, GG Pereira and M Warner Phys.

24 Jun 2012: We find a new FQHstate at 1, which does not exist without the pairing. ... Following [19] we switch to a new basis c ks ðc k0 þsic k1Þ=.

26 Jan 2012: Both sublatticesare also related by a magnetic translation involving a gaugetransformation.) The projection onto the lowest band real-izes a new effective problem on a triangular lattice visual-ized in Fig. ... 19] F. Gerbier and J. Dalibard, New J. Phys.

26 Jan 2012: Non-Abelian FQH states represent entirely new phasesof matter and could potentially be used for topologically-protected quantum computation (TQC) [20,21].

10 Oct 2012: Purcell)of new methods for nuclear magneticprecision measurements and discov-eries in connection therewith. ... zB 7! SzB, i.e. when represented. in terms of the new operators, the Néel ground state looks like a ferromagnetic state,with all spins

10 Oct 2012: 9] R. P. Feynman and A. R. Hibbs, Quantum Mechanics and Path Integrals, McGraw-Hill, New York, (1965). ... 10] R. P. Feynman, Statistical Mechanics, Benjamin, New York, (1972). Another classictext.

10 Oct 2012: What can be said aboutthe features of these new objects? First, they are structureless, i.e. ... within the new picture, ↠is an operator that createsparticles. The total energy of these states is given by!

5 Mar 2012: bond bya ‘diamond’ of new bonds.