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Atomic Physics at Accelerators: Mass Spectrometry - Proceedings of the APAC 2000, held in Cargese, France, 19-23 September 2000 (Hardcover, Reprinted from HYPERFINE INTERACTIONS, 132:1-4, 2001)
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Atomic Physics at Accelerators: Mass Spectrometry - Proceedings of the APAC 2000, held in Cargese, France, 19-23 September 2000 (Hardcover, Reprinted from HYPERFINE INTERACTIONS, 132:1-4, 2001)
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The search for examples of proton radioactivity has resulted in the
discovery of a large number of proton emitters in the region 50
< Z < 84 [1]. Many of these proton emitters and their
daughters are also a-emitters, and in some cases the a-decay chain
from the daughter terminates on a nuclide closer to stability whose
mass excess is known. This opens up the possibility of using a-and
proton-decay Q-values to determine the mass excesses of a large
group of nuclei connected by particle decay. The Q-values are
derived from the measured kinetic energies of the emitted protons
or a-particles. Where the decay chains are not connected to nuclei
with known mass excesses, proton separation energies can be
measured in some cases and derived in others. For the a-decay ofthe
parent nucleus (Z, A) to the daughter (Z - 2, A - 4), the energy
and momentum relations used to convert between Q-value, mass (M)
and mass excess (ME) are: M(4He)E", (1) M(Z - 2, A - 4)Erecoil, (2)
Q", E", + Erecoi\, ME(Z, A) Q", + ME(Z - 2, A - 4) + ME(4He). (3)
In practice, one uses M(4He) ~ 4 and M(Z - 2, A - 4) (A - 4), so
that Equation (3) becomes ME(Z, A) = E", (_A_) + ME(Z - 2, A - 4) +
ME(4He). (4) A -4 Similarly, for protons, we have ME(Z, A) =
Ep(_A_) +ME(Z - 1, A-I) +ME(lH).
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