![arXiv:1705.06742v1 [cond-mat.quant-gas] 18](http://s1.studyres.com/store/data/015536624_1-695304017ec91e58c90e68ba3242255c-300x300.png)
arXiv:1705.06742v1 [cond-mat.quant-gas] 18
... in insulating quantum magnets15–17 that possess wellisolated, quasi-one-dimensional chains of S = 1 local moments. Interestingly, ultracold atomic gases are a natural platform for realizing the complementary ferromagnetic spin-1 chain (cos θ < 0), where the system is an effective description of the ...
... in insulating quantum magnets15–17 that possess wellisolated, quasi-one-dimensional chains of S = 1 local moments. Interestingly, ultracold atomic gases are a natural platform for realizing the complementary ferromagnetic spin-1 chain (cos θ < 0), where the system is an effective description of the ...
Topological Order and the Kitaev Model
... many body interacting system defined over a 2-dimensional lattice. It exhibits the features of a topologically order system as its ground state is 4-fold degenerate when the lattice is embedded on the surface of a Torus, hence part of its name. The degeneracy is protected from local perturbations th ...
... many body interacting system defined over a 2-dimensional lattice. It exhibits the features of a topologically order system as its ground state is 4-fold degenerate when the lattice is embedded on the surface of a Torus, hence part of its name. The degeneracy is protected from local perturbations th ...
as a PDF
... We can easily see that there can be no overflows, since the carry outputs from the two quantum half adders contributing to the Sn-1 output cannot both be one. The sum out of the first will be zero if its carry is one, and the carry from the second cannot be one if the first half-adder’s sum is zero. ...
... We can easily see that there can be no overflows, since the carry outputs from the two quantum half adders contributing to the Sn-1 output cannot both be one. The sum out of the first will be zero if its carry is one, and the carry from the second cannot be one if the first half-adder’s sum is zero. ...
Preprint
... narrow resonance when the difference frequency between the two laser beams was varied (upper and middle part). The width of the resonance is caused by Doppler broadening and is therefore proportional to the condensate’s momentum uncertainty ∆p. It was determined for various sizes ∆x of the condensat ...
... narrow resonance when the difference frequency between the two laser beams was varied (upper and middle part). The width of the resonance is caused by Doppler broadening and is therefore proportional to the condensate’s momentum uncertainty ∆p. It was determined for various sizes ∆x of the condensat ...
Vibration Dynamics
... in which, x is a column array of describing coordinates of the system, and f is a column array of the associated applied forces. The square matrices [m], [c], [k] are the mass, damping, and stiffness matrices. Example 30 (The one, two, and three DOF model of vehicles) The one, two, and three DOF mod ...
... in which, x is a column array of describing coordinates of the system, and f is a column array of the associated applied forces. The square matrices [m], [c], [k] are the mass, damping, and stiffness matrices. Example 30 (The one, two, and three DOF model of vehicles) The one, two, and three DOF mod ...
Chapter 24 Physical Pendulum
... final potential energy for the two cases is plotted in Figures 24A.2 for −π < θ < π on the left and −π / 2 < θ < π / 2 on the right (the vertical scale is in units of mgl ). ...
... final potential energy for the two cases is plotted in Figures 24A.2 for −π < θ < π on the left and −π / 2 < θ < π / 2 on the right (the vertical scale is in units of mgl ). ...
Infrared and ultraviolet cutoffs of quantum field theory
... ∼ 10 eV. Other tests of QED, like shifts of energy levels in hydrogen atom, positronium, etc, lead in this case to less stringent bounds on the scale λ. The previous bound on the IR scale corresponds to an UV scale Λ < ∼ 10 TeV which is very close to the present and near future energies available in ...
... ∼ 10 eV. Other tests of QED, like shifts of energy levels in hydrogen atom, positronium, etc, lead in this case to less stringent bounds on the scale λ. The previous bound on the IR scale corresponds to an UV scale Λ < ∼ 10 TeV which is very close to the present and near future energies available in ...
