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Atomic Physics at Accelerators: Mass Spectrometry

Proceedings of the APAC 2000, held in Cargèse, France, 19–23 September 2000

  • Conference proceedings
  • © 2001

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Table of contents (64 papers)

  1. Tutorial on aspects of atomic masses (in honor of the 78th birthday of Aaldert Wapstra)

  2. Mass measurements and nuclear structure

  3. Mass measurements for metrology

  4. On-line ion trap mass measurement programs

Keywords

About this book

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).

Editors and Affiliations

  • CSNSM-IN2P3-Université de Paris Sud, Orsay, France

    David Lunney, Georges Audi

  • GSI, Darmstadt, Germany

    H.-Jürgen Kluge

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