Bloch excitations

Theoretical level populations. Sinee there are population variations on time seale shorter than some level lifetimes, a complete description of the excitation has been modeled solving optical Bloch equations Beacon model, Bellenger, 2002) at CEA. The model has been compared with a laboratory experiment set up at CEA/Saclay (Eig. 21). The reasonable discrepancy when both beams at 589 and 569 nm are phase modulated is very likely to spectral jitter, which is not modeled velocity classes of Na atoms excited at the intermediate level cannot be excited to the uppermost level because the spectral profile of the 569 nm beam does not match the peaks of that of the 589 nm beam. 

In the DC-biased structures considered here, the dynamics are dominated by electronic states in the conduction band [1]. A simplified version of the theory assumes that the excitation occurs only at zone center. This reduces the problem to an n-level system (where n is approximately equal to the number of wells in the structure), which can be solved using conventional first-order perturbation theory and wave-packet methods. A more advanced version of the theory includes all of the hole states and electron states subsumed by the bandwidth of the excitation laser, as well as the perpendicular k states. In this case, a density-matrix picture must be used, which requires a solution of the time-dependent Liouville equation. Substituting the Hamiltonian into the Liouville equation leads to a modified version of the optical Bloch equations [13,15]. These equations can be solved readily, if the k states are not coupled (i.e., in the absence of Coulomb interactions). 

All tensor expressions (35)-(42) involve summation over Bloch waves, i.e. summation over j. For a dynamical diffraction calculation involving AT beams, the number of Bloch waves resulting from Equation (30) equals the number of beams, i.e. N. It should be noted, however, that not all of these Bloch waves will be strongly excited within the crystal and contribute to the electron wave field. The excitation amplitudes of the Bloch waves in the crystal are given by B 0J. Extensive numerical calculations show that in a typical dynamical diffraction calculation, although typically more than... 

To verify the theory of PIP, a computer program using C language was developed. It can be used to directly calculate the excitation profiles by PIPs or any other RF pulses. The calculation is based on the Bloch vector model for a non-interacting spin-1/2 system, where the spin-lattice relaxation during the pulse is neglected. The basic idea of the program is discussed as follows. 

Finally - and equally important - Jens contribution to the formal treatment of GOS based on the polarization propagator method and Bethe sum rules has been shown to provide a correct quantum description of the excitation spectra and momentum transfer in the study of the stopping cross section within the Bethe-Bloch theory. Of particular interest is the correct description of the mean excitation energy within the polarization propagator for atomic and molecular compounds. This motivated the study of the GOS in the RPA approximation and in the presence of a static electromagnetic field to ensure the validity of the sum rules. 

The frequency ranges for maximum and minimum excitation can be exchanged, when the phases of successive pulses are alternating (Fig. 6a, version I vs. II). Since experiments were carried out at 1.5 T, theoretical calculations were based on intervals of 2.32 ms between consecutive pulses. Transverse magnetization in Fig. 6b was calculated by a program simulating Bloch s equations. 

Figure 4.18 The effect of spherical incident waves on the excitation of Bloch waves, (a) Reciprocal space the divergent incident beam has wavevectors ranging from P j O to P 2 O. (b) Real space energy is distributed throughout the Borrmann fan ABC. The beams generated outside the crystal are indicated...

The Bloch theorem is one of the tools that helps us to mathematically deal with solids [5,6], The mathematical condition behind the Bloch theorem is the fact that the equations which governs the excitations of the crystalline structure such as lattice vibrations, electron states and spin waves are periodic. Then, to jsolve the Schrodinger equation for a crystalline solid where the potential is periodic, [V(r + R) = V(r), this theorem is applied [5,6],... 

Karl Unterrainer, Photon-Assisted Tunneling in Semiconductor Quantum Structures P. Haring Bolivar, T. Dekorsy, and H. Kurz, Optically Excited Bloch Oscillations-Fundamentals and Application Perspectives... 

A typical spectrum was acquired with Bloch decays excited by 4 ysec pulses separated by 10 second recovery delays, and the data should give a reasonably quantitative estimate of the Si content. Previous work on other types of zeolites has demonstrated the importance of checking for complete relaxation if the spectra are to be used for quantitative studies. 

For the system in Fig. la, we assume that excitation induced by the circularly-polarized light produces a Bloch-type state on the donor ... 

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