Rabi expression

To solve this equation one needs an integrable expression for both / 12(f) and for D t). We used for the former the well-known Rabi expression which is valid for constant potential coupling Hu and for a constant energy gap. Note that the Rabi expression is derived with a quasi-diabatic basis set. Therefore the coupling appears through the potential coupling term (and X>i,2 = 0). 

The genes of the inducible and the constitutively expressed forms of NOS have been cloned and expressed. The expression of inducible NOS in the brain tissue of animals with experimentally induced neurological disorders (boma disease virus and rabies virus in rats), herpes simplex virus (mice) and experimental allergic encephalitis (in rats) suggests that NO produced by induced NOS may be a toxic fector in the pathogenesis of neurological diseases (Koprowski et /., 1993). 

Note that this expression may be considered as a consequence of the well-known Rabi equations. One may show easily that the two first moments of the undamped spectra are... 

Yusibov et al. [71] delivered to 14 human volunteers spinach expressing epitopes from the rabies virus glycoprotein and nucleoprotein fused to the coat protein of alfalfa mosaic virus (AlMV). Five of the fourteen subjects had previously received a... 

The strength of certain viral vaccines is expressed as international units (IU), which are based on animal potency tests (e.g., rabies vaccine). 

This mixed classical/quantum expression is valid for classical nuclear behavior and, strictly speaking, for the case of direct two-site interaction rather than superexchange, as the Landau-Zener expression was derived from the time-dependent Schrodinger equation assuming a two-state (reactant/product) electronic system with direct coupling. Nevertheless, it becomes clear on physical grounds that the form of Eqs. 4-5 can serve to define an effective A in the superexchange case in terms of the Rabi precession frequency characteristic of the two trap sites embedded in the complex system wherein 2A/h would be computed from this net effective Rabi precession frequency. 

Monoclonal Antibodies Expressed in Plants against Rabies Virus... 

Ashraf, S., Singh, P.K., Yadav, D.K., Shahnawuz, M., Mishra, S., Sawant, S.V., and Tuli, R. (2005). High level expression of surface glycoprotein of rabies virus in tobacco and its immunoprotective activity in mice. J. Biotechnol. 119(1) 1-14. 

Yusibov, V., Hooper, D.C., Spitsin, S.V., Fleysh, N., Kean, R.B., Mikheeva, T., Deka, D., Karasev, A., Cox, S., Randall, J., and Koprowski, H. (2002). Expression in plants and immunogenicity of plant virus-based experimental rabies vaccine. Vaccine 20 3155-3164. 

Girard, L.S., Fabis, M.J., Bastin, M., Courtois, D., Petiard, V., and Koprowski, H. (2006). Expression of a human anti-rabies virus monoclonal antibody in tobacco cell cultnre. Biochem. Biophys. Res. Commun. 345(2) 602-607. 

These are discussed elsewhere but include a recombinant vaccinia virus that expresses rabies virus glycoproteins used for oral vaccination. 

We note that the lowest adiabatic state, Eq. (58), is expressed in terms of the initial and the final states without the intermediate state. This property implies that the system in the initial state is transferred to the final state adia-batically, with no population in the intermediate resonant state. That is, under the condition for the Rabi frequencies 2/>(0I 2s(0l, we can see from Eqs. (64) and (65)... 

Zhou D, Cun A, Li Y, Xiang Z, Ertl HC. A chimpanzee-origin adenovirus vector expressing the rabies virus glycoprotein as an oral vaccine against inhalation infection with rabies virus. Mol Ther 2006 14 662-72. 

This chapter is organized as follows. In Section II, we show how quantum chaos systems can be controlled under the optimal fields obtained by OCT. The examples are a random matrix system and a quantum kicked rotor. (The former is considered as a strong-chaos-limit case, and the latter is considered as mixed regular-chaotic cases.) In Section III, a coarse-grained Rabi state is introduced to analyze the controlled dynamics in quantum chaos systems. We numerically obtain a smooth transition between time-dependent states, which justifies the use of such a picture. In Section IV, we derive an analytic expression for the optimal field under the assumption of the CG Rabi state, and we numerically show that the field can really steer an initial state to a target state in random matrix systems. Finally, we summarize the chapter and discuss further aspects of controlling quantum chaos. 

Lamb, of course, was thoroughly familiar with Rabi s molecular beam experiments, and Lamb s experimental design drew ftom the Rabi beam approach. The objective of Lamb s experiment is clearly expressed in a progress report he wrote in 1946 ... 

The results of a series of measurements such as those shown in Fig. 9 are shown in Fig. 10. It is clear that the observed Rabi frequencies are in excellent agreement with the Bessel function expression of Eq. (10). In particular, it is interesting to note that the zeros in the Bessel function are reproduced in the experimental data. These data show clearly that the Floquet description presented above is indeed accurate for Rydberg atoms in continuous wave micro-wave fields. 

This approximation becomes exact in the case of resonant Rabi oscillations (Tr = 0, uia = lum), which explains why the QZE is observable in Itano s experiment [Itano 1990] for any v. More generally, this approximation holds for any G uf) that falls off faster than 1/uj on the wings. Then our universal expression yields the most general result for the QZE, namely that R decreases with v. 

When the photons are linearly polarized, the Rabi frequencies = ( d p)/27i coincide with the above defined Rabi frequencies. We assume real transition dipole moments and amplitudes of the electromagnetic fields and use the following expressions for the field amplitudes, = fit/cen. = Jlle/ceQ. Here = e , > = e> e and e are the polarization vectors of strong pump and ASE fields. 

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