Strong-Disorder Fixed Point in the Dissipative Random Transverse-Field Ising Model
... i are Pauli matrices and the masses of the oscillators are set to one. The quenched random bonds Ji (and transverse fields hi ) are uniformly distributed in 0; J0 and 0; h0 , respectively. The properties of the bath are speciP fied by its spectral function Ji ! 2 ki C2ki =!ki ! !ki ...
... i are Pauli matrices and the masses of the oscillators are set to one. The quenched random bonds Ji (and transverse fields hi ) are uniformly distributed in 0; J0 and 0; h0 , respectively. The properties of the bath are speciP fied by its spectral function Ji ! 2 ki C2ki =!ki ! !ki ...
Research Article Mathematical Transform of Traveling
... momentum of the quantum particle see 10 for more details. The quantities Aeμ x and Aeμ p do not correspond to standard photons, and for this reason they cannot be substituted by operators as required by second quantification theory. However, experimental facts have shown that the electromagn ...
... momentum of the quantum particle see 10 for more details. The quantities Aeμ x and Aeμ p do not correspond to standard photons, and for this reason they cannot be substituted by operators as required by second quantification theory. However, experimental facts have shown that the electromagn ...
The Structure of the Atom
... He has 2 electrons, can we add another electron spinning in another direction in the first energy level of the s sublevel with its 1 spherical orbital? No, the third electron must go to the 2nd energy level which has 2 sublevels, s and p, s with its one spherical orbital and p with its 3 orientation ...
... He has 2 electrons, can we add another electron spinning in another direction in the first energy level of the s sublevel with its 1 spherical orbital? No, the third electron must go to the 2nd energy level which has 2 sublevels, s and p, s with its one spherical orbital and p with its 3 orientation ...
Non-equilibrium steady state of sparse systems OFFPRINT and D. Cohen D. Hurowitz
... Fig. 6: (Colour on-line) The dependence of T∞ on the width σ of the log-normal distribution. Note that the sparsity is s = exp(−σ 2 ). We confirm that T∞ is bounded from below by [Δ(En )/Δ(Er )]TB (dashed red line), and tends to TB in the sparse limit. Here Δ(En ) = 25 is the width of energy window i ...
... Fig. 6: (Colour on-line) The dependence of T∞ on the width σ of the log-normal distribution. Note that the sparsity is s = exp(−σ 2 ). We confirm that T∞ is bounded from below by [Δ(En )/Δ(Er )]TB (dashed red line), and tends to TB in the sparse limit. Here Δ(En ) = 25 is the width of energy window i ...
Time-dependent quantum circular billiard
... by Makowski et al. [16]. We solve the Schr¨odinger equation for the circular billiard with a time-dependent radius. In particular, we consider the following cases: i) monotonically expanding (contracting) circle; ii) non-harmonically breathing circle; iii) harmonically breathing circle. The classica ...
... by Makowski et al. [16]. We solve the Schr¨odinger equation for the circular billiard with a time-dependent radius. In particular, we consider the following cases: i) monotonically expanding (contracting) circle; ii) non-harmonically breathing circle; iii) harmonically breathing circle. The classica ...
Experimental one-way quantum computing
... Standard quantum computation is based on sequences of unitary quantum logic gates that process qubits. The one-way quantum computer proposed by Raussendorf and Briegel is entirely different. It has changed our understanding of the requirements for quantum computation and more generally how we think ...
... Standard quantum computation is based on sequences of unitary quantum logic gates that process qubits. The one-way quantum computer proposed by Raussendorf and Briegel is entirely different. It has changed our understanding of the requirements for quantum computation and more generally how we think ...
