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Double-p Decay

The periodic variation of the mass surface caused by the pairing energy also causes a large number of even-even nuclei to be unstable with respect to two [Pg.217]

Two reactions have been studied as possible candidates for double-(3 decay. The first reaction is simply two times the normal (3 decay process  [Pg.218]

Instrumental searches for this latter neutrinoless process have been made, but there is no strong evidence for its existence. The former two-neutrino decay has been observed with a variety of techniques that were carefully tuned to detect the rare products. [Pg.218]

The first term is the constant 8 x 1020/s and the second term reflects the details of the decay. Using M = /2 for the decay from the 0+ ground state, to the 0+ ground state of the daughter, the second term is 1.5 x 10-25/. For this case, log(/) 1.5, then taking the first term times the square of the second for double-(3 decay, we get A 10-26/s, or 10 19 per year Given that a mole of this gas has 1024 atoms, we expect about one decay per day in the entire sample. [Pg.218]

Sketch quantitatively the shape of the neutrino energy spectrum for the following types of decay. Label all axes carefully and indicate the types of neutrinos involved. [Pg.219]


There are four modes of radioactive decay that are common and that are exhibited by the decay of naturally occurring radionucHdes. These four are a-decay, j3 -decay, electron capture and j3 -decay, and isomeric or y-decay. In the first three of these, the atom is changed from one chemical element to another in the fourth, the atom is unchanged. In addition, there are three modes of decay that occur almost exclusively in synthetic radionucHdes. These are spontaneous fission, delayed-proton emission, and delayed-neutron emission. Lasdy, there are two exotic, and very long-Hved, decay modes. These are cluster emission and double P-decay. In all of these processes, the energy, spin and parity, nucleon number, and lepton number are conserved. Methods of measuring the associated radiations are discussed in Reference 2 specific methods for y-rays are discussed in Reference 1. [Pg.448]

The observation of double P-decay has been of particular interest because there are different concepts of how this decay can occur. The theoretical half-life depends on what concept is correct. Also, the predictions of the theory influence not only the design of the experiments used to observe the decay, but also the interpretation. [Pg.452]

PP2- However, there is an alternative theoretical mechanism by which the two Ps could be emitted without any neutriao, denoted PPq- The experimental methods that are used to look for the double P decay mode are often more sensitive to one of these decay modes than the other. The difference ia the expected energy distribution of the electrons is clear from the fact that ia the first case the total decay energy is divided between four particles, including the two antineutfinos that caimot be observed ia the second, it is only divided between the two electrons. As more exotic modes of decay are measured and even larger limits are placed on some of the half-fives, the constraints on theory become even stronger. [Pg.453]

Although ot, p, and y decay are the most common decay modes, several others exist, including fission, delayed neutron and proton emission, double-P decay, 2-proton decay, and decay by emission of heavier particles. Among these, fission is probably the most important in terms of its industrial and defense applications, and ancillary waste concerns. [Pg.7]

See also P-decay half-life results for, 21 3071 Double bonds... [Pg.288]

Masters. P.M. and M.R. Zimmerman Age Determination of an Alaskan Mummy Morphological and Biochemical Correlation." Science, 2U1. 811-812 (1978). Moe, M.K. and S.P. Rosen Double-Beta Decay," Sci. Amer.. 48 (November 1989). Monastersky. K. "Coral Corrects Carbon Daring Problems, Science News, 356 (June 9, i 990). [Pg.1416]

Decay modes are a = alpha particle emission (B = negative beta emission p+ = positron emission EC = orbital electron capture IT = isomeric transition from upper to lower isomeric state n = neutron emission sf = spontaneous fission (B(B = double beta decay. Total disintegration energy in MeV units. [Pg.1796]

Because there is a double decay involved in parent P disintegration, the decay equation corresponding to the general formula of equation 11.83 reads as follows ... [Pg.747]

The overpotentia] measured at a current density of 10-5 A/cm2 was +0.236 V. The decay of the overpotential with the cut off of the current was observed as listed Table P.l. Calculate the double-layer capacitance, the exchange current density, and the transfer coefficient for the electrochemical reaction. (Kim)... [Pg.731]


See other pages where Double-p Decay is mentioned: [Pg.442]    [Pg.452]    [Pg.288]    [Pg.288]    [Pg.217]    [Pg.517]    [Pg.28]    [Pg.34]    [Pg.118]    [Pg.442]    [Pg.452]    [Pg.288]    [Pg.288]    [Pg.217]    [Pg.517]    [Pg.28]    [Pg.34]    [Pg.118]    [Pg.96]    [Pg.182]    [Pg.617]    [Pg.704]    [Pg.78]    [Pg.144]    [Pg.88]    [Pg.182]    [Pg.113]    [Pg.276]    [Pg.119]    [Pg.12]    [Pg.310]    [Pg.403]    [Pg.242]    [Pg.3]    [Pg.133]    [Pg.145]    [Pg.399]    [Pg.676]    [Pg.24]    [Pg.441]    [Pg.42]    [Pg.132]    [Pg.306]    [Pg.41]    [Pg.399]    [Pg.324]   


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Double 3 decay

P-doubling

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