Quantum information with Rydberg atoms
... C-Phase/C-NOT: same operations, but only carried out of ”control-qubit” is in state |0>. ...
... C-Phase/C-NOT: same operations, but only carried out of ”control-qubit” is in state |0>. ...
Magneto-optical properties of charged excitons in quantum dots
... the peak positions of the upper and lower branches shown left plotted against positive and negative B, respectively. The solid line is a fit of the energy to a second order polynomial in B. ...
... the peak positions of the upper and lower branches shown left plotted against positive and negative B, respectively. The solid line is a fit of the energy to a second order polynomial in B. ...
Paper
... At a fixed value for temperature, in MC simulations, the quantum effects at the second order in ћ are taken into account by substituting the pair potential UC(r) by the UQFH(r). MD simulations, equivalent to MC simulations made with a QFH potential, are easily realized by using a MD simulation metho ...
... At a fixed value for temperature, in MC simulations, the quantum effects at the second order in ћ are taken into account by substituting the pair potential UC(r) by the UQFH(r). MD simulations, equivalent to MC simulations made with a QFH potential, are easily realized by using a MD simulation metho ...
A New Approach to the ⋆-Genvalue Equation
... which are similar to those satisfied by the Heisenberg–Weyl operators. These facts (z 0 , t) = e it T (z 0 ) defines a unitary representation of the Heisenberg suggest that T group. Let us prove this is indeed the case. For this we will need the linear mapping Wφ : S(Rn ) −→ S(R2n ) defined by Wφ ...
... which are similar to those satisfied by the Heisenberg–Weyl operators. These facts (z 0 , t) = e it T (z 0 ) defines a unitary representation of the Heisenberg suggest that T group. Let us prove this is indeed the case. For this we will need the linear mapping Wφ : S(Rn ) −→ S(R2n ) defined by Wφ ...
Non-Equilibrium Quantum Many-Body Systems: Universal Aspects
... ⇒ Broadening of Fermi surface delayed to times ∝ tR2 ...
... ⇒ Broadening of Fermi surface delayed to times ∝ tR2 ...
3.3.3: Semi-Lagrangian schemes
... wave number generated in a quadratic term can be pmax’=2π which can not be presented in the grid. ...
... wave number generated in a quadratic term can be pmax’=2π which can not be presented in the grid. ...
Ch3-3-3&4_Hong
... wave number generated in a quadratic term can be pmax’=2π which can not be presented in the grid. ...
... wave number generated in a quadratic term can be pmax’=2π which can not be presented in the grid. ...
Temporal Coherence of Photons Emitted by Single Nitrogen
... sublevel being much smaller than those from mS 1 sublevels. The rates of ISC transitions towards the groundstate triplet 1 A ! 3 A are also spin selective, but here the mS 0 state is mostly populated. Hence after a few optical excitation emission cycles a strong spin polarization of the ground- ...
... sublevel being much smaller than those from mS 1 sublevels. The rates of ISC transitions towards the groundstate triplet 1 A ! 3 A are also spin selective, but here the mS 0 state is mostly populated. Hence after a few optical excitation emission cycles a strong spin polarization of the ground- ...
Impulse and Momentum
... equal velocity. This is known as the period of deformation. Following this, the particles will either remain deformed, or return to their original shape, referred to as the period of restitution. These are demonstrated below. ...
... equal velocity. This is known as the period of deformation. Following this, the particles will either remain deformed, or return to their original shape, referred to as the period of restitution. These are demonstrated below. ...
