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Alpha particle clustering

Knockout reactions, such as (p,a), and (e,e a) in even N= Z (alpha particle) nuclei are also especially important as they provide evidence for alpha particle clustering in nuclei. At low energies, such reactions, for example, F(p,a) and Si(y,a) Mg, which reduce the mass of... [Pg.187]

Abstract The equation of state (EOS) of nuclear matter at finite temperature and density with various proton fractions is considered, in particular the region of medium excitation energy given by the temperature range T < 30 MeV and the baryon density range ps < 1014 2 g/cm3. In this region, in addition to the mean-field effects the formation of few-body correlations, in particular light bound clusters up to the alpha-particle (1 < A < 4) has been taken into account. The calculation is based on the relativistic mean field theory with the parameter set TM1. We show results for different values for the asymmetry parameter, and (3 equilibrium is considered as a special case. [Pg.75]

Z18Ra corresponding to 8% of the El molecular sum rule [8] In Z °Ra an enhanced ground state alpha particle decay width is already known and the systematics of the Ra isotopes suggest a decrease in the alpha hindrance factors for the 1 and 3 states--as predicted by the cluster model. [Pg.284]

Lind bases his cluster-ion theory on these results with alpha particles. Each ion attaches one or more neutral molecules of the reacting substances and when the ions are neutralized all the molecules involved in the two clusters undergo chemical reaction. The M/N ratio gives a measure of the number of neutral molecules... [Pg.189]

The experimenters set up a lead-shielded box containing radioactive polonium, which emitted a beam of positively charged subatomic particles through a small hole. Today, we know that the particles of the beam consisted of clusters containing two protons and two neutrons and are called alpha particles. The sheet of gold foil was surrounded by a screen coated with zinc sulfide, which glows when struck by the positively charged particles of the beam. [Pg.64]

Fig. 15. Plot of methanol preference factor > in mixed protonated water-methanol clusters. Circles 5 and 2.5 Torr total pressure results obtained with an alpha-particle mass spectrometer Squares data from proton-beam mass spectrometer. Extrapolation leads to preference for water above n = 9. Fig. 15. Plot of methanol preference factor > in mixed protonated water-methanol clusters. Circles 5 and 2.5 Torr total pressure results obtained with an alpha-particle mass spectrometer Squares data from proton-beam mass spectrometer. Extrapolation leads to preference for water above n = 9.
When a radioactive nuclide decays, electrons are stripped from the parent atom by its recoil and decay products are formed as positive ions. These ions can attract liquid and even solid material, thus forming clusters of atoms or particles in the submicron region ranging from 0.001 to 0.01 pm. Air is permanently ionised by radiation from the natural radioactivity of air and by cosmic radiation which consists mostly of positively charged particles, 85% protons, 10% alpha particles with a smaller percentage of positively charged stripped nuclei of heavier elements, such as Fe, Co and Ni, etc. Production of an ion pair requires 35.6 eV if ionisation is by alpha particles and 32.5 eV if by fast electrons. In the free atmosphere, the rate of production of small ions is in balance with the rate of neutralisation by recombination and the rate of attachment to condensation nuclei. Condensation nuclei are mostly the Aitken nuclei, which are submicrometre particles in the range 0.005 to 0.01 pm. [Pg.6]

Both polonium nuclides are alpha emitters and therefore of particular concern. In health physics it is customary to differentiate between attached and unattached 218Po the former, usually the larger of the two consists of 218Po atoms attached to airborne particles which are copiously present in virtually every atmosphere the latter consists of a 218Po atom or ion, frequently surrounded by several dozen molecules of a condensible species present in the air. The purpose of this paper is to present a new method for measuring the size properties of these unattached 218Po clusters. [Pg.344]

Evidence, based on recent (n,n y) reaction experiments and previous particle transfer studies is presented in support of a coexisting four-particle, four-hole band built on the 1581-keV first excited 0+ state in the doubly closed subshell nucleus 9 >Zr. An alternative explanation for this band in terms of alpha-clustering appears reasonable. [Pg.200]


See other pages where Alpha particle clustering is mentioned: [Pg.272]    [Pg.213]    [Pg.272]    [Pg.213]    [Pg.212]    [Pg.216]    [Pg.164]    [Pg.37]    [Pg.176]    [Pg.506]    [Pg.176]    [Pg.641]    [Pg.273]    [Pg.281]    [Pg.281]    [Pg.282]    [Pg.176]    [Pg.45]    [Pg.182]    [Pg.508]    [Pg.4]    [Pg.316]    [Pg.321]    [Pg.171]    [Pg.212]    [Pg.1861]    [Pg.37]    [Pg.363]    [Pg.239]    [Pg.404]    [Pg.676]    [Pg.264]    [Pg.369]    [Pg.302]    [Pg.133]    [Pg.50]    [Pg.746]    [Pg.168]    [Pg.603]    [Pg.410]   
See also in sourсe #XX -- [ Pg.187 , Pg.213 ]




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