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Cold neutrons

SANS Small-angle neutron scattering [175, 176] Thermal or cold neutrons are scattered elastically or inelastically Incident-Beam Spectroscopy Surface vibrational states, pore size distribution suspension structure... [Pg.316]

There is a narrow regime near the points (K =125 MeV. t=2.5) and (Kq=200 MeV, t=2) that permits a successful explosion. However, as Baron et al. themselves realize, these values for the EOS parameters are ruled out by the masses observed for cold neutron stars, if the EOS of neutron-star matter is not stiffer than our EOS. [Pg.419]

In the late twentieth eentury, a number of new instrumental techniques w erc developed lor determining atomic properties with increased precision and reliability. Of marked importance is the Increased facility for measuring minute dimensions and units of time at the respective nanometer and nanosecond levels. Laboratory techniques include laser atom probes, cold neutron research, .canning-tunneling microscopy, and atom trapping, among others. [Pg.347]

During the past decade, since their detection, much research has been directed toward methods of extracting, storing, and manipulating ultra-cold neutrons. It now appears that the next period will be one of investigating die neutron per se and possibly of using this new knowledge for the study of other systems of particles. [Pg.1068]

The first was a brief note in 1956 on the possibility of cold neutron storage [15 ]. It is known that a neutron moving with sufficiently small velocity experiences complete internal reflection in its fall from a vacuum to a wall... [Pg.36]

The storage of cold neutrons (the idea and the experiment) was registered officially as a discovery in 1958. Ya.B. was awarded the Kurchatov gold medal for this work. [Pg.37]

Figure 5. The measured attenuation coefficient for die NIST MCP detector at die BT2 thermal neutron beam and the NG1 cold neutron beam. Figure 5. The measured attenuation coefficient for die NIST MCP detector at die BT2 thermal neutron beam and the NG1 cold neutron beam.
A.S Tremsin., J.V. Vallerga, J.B. McPhate, et al., On the possibility to image thermal and cold neutron with sub- 15 pm spatial resolution. Nucl. Instrum. Methods, Sect. A 592, 374-384 (2008)... [Pg.200]

Cold neutrons <0.01 Low scattering good detection, high absorption cross-section results in decreased transparency of samples... [Pg.133]

The potential of PGAA can best be explored when guided beams of cold neutrons are used because the cross section of (n,y) can increase significantly. [Pg.209]

Larsson, K. E., U. Dahlborg, and D, Jovic Collective Atomic Motions in Liquid Aluminium studied by Cold Neutron Scattering. Wien, Int. Atom. Energy Agency 1964. [Pg.99]

O Reactor core Hot neutrons Thermal neutrons Cold neutrons... [Pg.6141]

Figure 2 Layout of the Institute Laue Langevin (Grenoble, France) Research Reactor Instrumentation including two cold neutron gnide halls... Figure 2 Layout of the Institute Laue Langevin (Grenoble, France) Research Reactor Instrumentation including two cold neutron gnide halls...
An interesting application of neutron scattering techniques is the use of neutrons to determine the validity of artifacts. Because neutron scattering (specifically using thermal to cold neutrons) is a nondestructive technique, it can be utilized to probe sensitive, priceless artifacts. Leever etalf used the GEM neutron diffractometer at ISIS to do a comparative, structural analysis of two harquebusier breastplates. In the study, it was determined that the structural makeup of the two breastplates was different hence one was verified to date around 1600-1650 a.d., while the other was a replica from the late 19th century. [Pg.6156]

J. Z. Larese, Neutron Scattering Investigations of the Dynamics of Thin Films Adsorbed on Solid Surfaces, Materials Research Using Cold Neutrons at Pulsed Neutron Sources, [Proceedings] , Argonne, Aug. 25-26, 1997, 1999, p. 57. [Pg.6160]

SANS has historically been the domain of cold neutrons on reactor based sources, and impressive instrumentation, such as notably D22 at the Institute Laue Langevin, is currently available. The more recent emergence of neutron reflectivity as a probe of surface structure has been very much linked to the development of pulsed neutron sources and much of the initial impact of this technique has arisen from pulsed source instrumentation, such as the CRISP and SURF reflectometers at ISIS. - ... [Pg.276]

Potential developments in instrumentation and the neutron source at ISIS (Second Target Station optimised for cold neutrons) will be discussed, and the longer term potential of the European Spallation Source, ESS, presented. [Pg.277]

An early investigation of the low-frequency vibrations of polyethylene by the cold neutron scattering technique was reported by Zemlyanov and Cheenoplekov (47), who made measurements, at 20° C, on low-density polyethylene, before and after irradiation to induce crosslinking. They reported maxima at wavelengths of 1.51, 1.78, 2.04, 2., 2.63, and 2.94 A. Changes in the relative intensities of the latter three maxima were observed after the irradiation treatments. No attempt was made to interpret the spectra in terms of specific vibrational motions, or to correlate the results with theory. [Pg.10]

Golub, R., Richardson, D., and Lamoreaux, S.K. (1991) Ultra-Cold Neutrons, Adam Hilger Press, Boston. [Pg.185]

P.A. Egelstaff (1951). Nature, 168, 290. Inelastic scattering of cold neutrons. [Pg.11]

Fig. 3.5 Plan of the ISIS Facility (Chilton, UK) [8]. The major components are shown, INS instruments are indicated. TS-I is the high power 50 Hz target station and TS-II is the long wavelength, cold neutron 10 Hz target station. TS-II is scheduled to be operational in 2008. Fig. 3.5 Plan of the ISIS Facility (Chilton, UK) [8]. The major components are shown, INS instruments are indicated. TS-I is the high power 50 Hz target station and TS-II is the long wavelength, cold neutron 10 Hz target station. TS-II is scheduled to be operational in 2008.
FIGURE 6 Neutron spectra for o-xylene measured by small k and cold neutron techniques. [Pg.379]

Early in the development of the theory of nucleosynthesis, an alternative to the high-T r-process canonical model (Sects. 7.1 and 7.2) has been proposed [63], It relies on the fact that very high densities (say p > 1010 gem-3) can lead material deep inside the neutron-rich side of the valley of nuclear stability as a result of the operation of endothermic free-electron captures, this so-called neutronisation of the material being possible even at the T = 0 limit. The astrophysical plausibility of this scenario in accounting for the production of the r-nuclides has long been questioned, and has remained largely unexplored until the study of the composition of the outer and inner crusts of neutron stars and of the decompression of cold neutronised matter resulting from tidal effects of a black hole on a neutron-star companion ([24] for references). The decompression of cold neutron star matter has recently been studied further (Sect. 9). [Pg.316]

As reminded in Sect. 7.3, the decompression of the crust of cold neutron stars (NSs) made of a lattice of very neutron-rich nuclei immersed in a gas of neutrons and degenerate electrons has long been envisioned as a possible site for the development of a high-density r-process (HIDER). This decompression could result from the coalescence of two NSs or of a NS and a black hole (BH) in a binary system. It could also result from the ejection of material from magnetars. [Pg.321]


See other pages where Cold neutrons is mentioned: [Pg.20]    [Pg.123]    [Pg.9]    [Pg.335]    [Pg.178]    [Pg.184]    [Pg.185]    [Pg.186]    [Pg.189]    [Pg.63]    [Pg.321]    [Pg.92]    [Pg.7]    [Pg.97]    [Pg.99]    [Pg.6141]    [Pg.18]    [Pg.286]    [Pg.286]    [Pg.288]    [Pg.27]    [Pg.184]    [Pg.80]    [Pg.376]    [Pg.382]    [Pg.205]    [Pg.792]   
See also in sourсe #XX -- [ Pg.1624 , Pg.1631 , Pg.1664 , Pg.1666 ]

See also in sourсe #XX -- [ Pg.425 , Pg.451 ]




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