Quantum motion of electrons in topologically distorted crystals
									
... of the ideal lattice and consequently leads to a breakdown of the Bloch theorem for electronic quantum states. Outside the core region of such topological defects the lattice locally looks perfect but globally is distorted at arbitrary distances from the core. One therefore expects that sufficiently ...
                        	... of the ideal lattice and consequently leads to a breakdown of the Bloch theorem for electronic quantum states. Outside the core region of such topological defects the lattice locally looks perfect but globally is distorted at arbitrary distances from the core. One therefore expects that sufficiently ...
									The Gutzwiller Density Functional Theory - cond
									
... : matrix of variational parameters (in this lecture problem: ...
                        	... : matrix of variational parameters (in this lecture problem: ...
									3.3 The time-dependent Schrödinger equation
									
... Schrödinger equation, with eigenenergy E is also a solution of the time-dependent equation as long as we always multiply it by a factor exp  iEt /   If   r  is a solution of the time-independent Schrödinger equation, with eigenenergy E then   r, t     r  exp  iEt /   is a solution ...
                        	... Schrödinger equation, with eigenenergy E is also a solution of the time-dependent equation as long as we always multiply it by a factor exp  iEt /   If   r  is a solution of the time-independent Schrödinger equation, with eigenenergy E then   r, t     r  exp  iEt /   is a solution ...
									8.514 Many-body phenomena in condensed matter and atomic
									
... where c is a scaling factor. The relation of coherent states with the points in a classical phase space will be clarified below. Let us find the form of a coherent state in the q-representation, ψυ (q) = < q | υ >. As before, we use the units in which the length λ=1, and write ...
                        	... where c is a scaling factor. The relation of coherent states with the points in a classical phase space will be clarified below. Let us find the form of a coherent state in the q-representation, ψυ (q) = < q | υ >. As before, we use the units in which the length λ=1, and write ...
									Mixed-State Evolution in the Presence of Gain and Loss
									
... that gain and loss can be balanced without perturbing the system, is possible. If, on the other hand, a coherent implementation of gain and loss is not feasible, either because of fundamental quantum limits or current technological limits, then it is important to take into account additional effects ...
                        	... that gain and loss can be balanced without perturbing the system, is possible. If, on the other hand, a coherent implementation of gain and loss is not feasible, either because of fundamental quantum limits or current technological limits, then it is important to take into account additional effects ...
									Long-range Rydberg-Rydberg interactions in calcium, strontium and
									
... case in general. In particular, many of the eigenstates of Ĥ (6) vary with n1 and n2 , unlike the eigenstates of Ĥ (5) . The correspondence between even and odd values of K and the symmetry under the interchange of the states of atoms 1 and 2 is nonetheless the same. In general, the composition of ...
                        	... case in general. In particular, many of the eigenstates of Ĥ (6) vary with n1 and n2 , unlike the eigenstates of Ĥ (5) . The correspondence between even and odd values of K and the symmetry under the interchange of the states of atoms 1 and 2 is nonetheless the same. In general, the composition of ...
									Advanced Atomic, Molecular and Optical Physics
									
... • Atoms are the best examples of quantum systems we have. • They can be prepared in very well defined states. • Their temporal evolution can be measured and manipulated. • Atomic physics experiments can be reproduced all over the world. • They deliver the most accurate results in any experimental sc ...
                        	... • Atoms are the best examples of quantum systems we have. • They can be prepared in very well defined states. • Their temporal evolution can be measured and manipulated. • Atomic physics experiments can be reproduced all over the world. • They deliver the most accurate results in any experimental sc ...