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Cooling Inelastic scattering

It is clear that cooling and loss processes compete and therefore the ratio of elastic to inelastic scattering becomes a crucial parameter dictating the survival times of anti-... [Pg.199]

As previously mentioned, the neutron economy is very important to realize long-life small reactors. For these, it is expected that LBE coolant has better performance in neutron economy than sodium coolant because of a larger elastic and smaller inelastic scattering cross section. It is reported that the LBE cooled long-life small fast reactor shows better performance for neutron economy, bum-up reactivity swing and void coefficient [XXV-3]. [Pg.717]

Figure 10.11 The logarithm ofthe N2 rotational population (corrected for nuclear spin statistics) is plotted against ] ] + 1), which is proportional to rotational energy, for inelastic scattering of N2 from the 111 surface of a silver crystal as a function of incident beam energy for an incident scattering angle of 15° and a final scattering angle of 20°, close to the specular direction. The N2 beam is supersonically cooled and has a rotational distribution that peaks at y = 0 and does not extend beyond j = 3. The surface temperature is 90 K [adapted from G. O. Sitz, A. C. Kummel, and R. N. Zare, J. Chem. Phys. 89, 2558 (1988)]. Figure 10.11 The logarithm ofthe N2 rotational population (corrected for nuclear spin statistics) is plotted against ] ] + 1), which is proportional to rotational energy, for inelastic scattering of N2 from the 111 surface of a silver crystal as a function of incident beam energy for an incident scattering angle of 15° and a final scattering angle of 20°, close to the specular direction. The N2 beam is supersonically cooled and has a rotational distribution that peaks at y = 0 and does not extend beyond j = 3. The surface temperature is 90 K [adapted from G. O. Sitz, A. C. Kummel, and R. N. Zare, J. Chem. Phys. 89, 2558 (1988)].
Figure 3 Phonon dispersion curves obtained by inelastic neutron scattering revealing precursor behaviour prior to the 14M transformation in Ni-AI. The dip at q = 1/6 [110] (a) deepens upon cooling and (b) shifts under an external load . Figure 3 Phonon dispersion curves obtained by inelastic neutron scattering revealing precursor behaviour prior to the 14M transformation in Ni-AI. The dip at q = 1/6 [110] (a) deepens upon cooling and (b) shifts under an external load .
We have evaluated the cross sections for the most important collisional processes in the H — H scattering, notably the cross sections for elastic scattering (leading to antihydrogen cooling), and for various inelastic processes (leading to the loss of antihydrogen). [Pg.197]

There have been several measurements of the lattice dynamics of quartz by inelastic neutron scattering. Early results showed that the soft mode in the high-temperature phase is overdamped (Axe 1971). Other work on RUMs at wave vectors not directly associated with the phase transition showed that on cooling through the phase transition the RUMs rapidly increase in frequency since they are no longer RUMs in the low-temperature phase (Boysen et al. 1980). The most definitive study of the RUMs associated with the phase transition was that of Dolino et al. (1992). [Pg.11]

In order to introduce the theory of vibrational spectroscopy in inelastic neutron scattering, we make some simplifications that will help us to understand the concepts. First we shall deal with the vibrational modes of molecules in a vacuum or in a dilute gas phase. Note, however, that in INS experiments the sample is cooled to ca 20 K, therefore the molecules are part of an extended solid. However, because the forces that keep the atoms in the molecule are often larger than the forces that molecules experience from other molecules in the condensed phase, isolated molecule calculations can be good models. [Pg.140]


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See also in sourсe #XX -- [ Pg.320 ]




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Inelastic scatter

Inelasticity

Scatter inelastically

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