2005 APS April Meeting
Saturday–Tuesday, April 16–19, 2005;
Tampa, FL
Session X11: Precision Measurements of Nucleons and Nuclei
10:45 AM–12:33 PM,
Tuesday, April 19, 2005
Marriott Tampa Waterside
Room: Room 7
Sponsoring
Unit:
DNP
Chair: Dave Mack, Jefferson National Laboratory
Abstract ID: BAPS.2005.APR.X11.3
Abstract: X11.00003 : Fundamental Symmetries Probed by Precision Nuclear Mass Measurements at ISOLTRAP
11:57 AM–12:33 PM
Preview Abstract
Abstract
Author:
Georg Bollen
(Michigan State University, National Superconducting Cyclotron Laboratory, East Lansing, MI, USA)
Mass measurements on rare isotopes can play an important role in testing the
nature of fundamental interactions. Precise mass values together with decay
data are required for critical tests of the conserved vector current (CVC)
hypothesis and the standard model. Substantial progress in Penning trap mass
spectrometry has made this technique the best choice for precision
measurements on rare isotopes, by providing high accuracy and sensitivity
even for short-lived nuclides. The pioneering facility in this field is
ISOLTRAP at ISOLDE/CERN. ISOLTRAP is a mass spectrometer capable to
determine nuclear binding energies with an uncertainty of 10$^{-8}$ on
nuclides that are produced with yields as low as a few 100 ions/s and at
half-lives well below 100 ms. It is used for mass measurements relevant for
a better understanding of nuclear structure and the nucleosynthesis of the
elements. It is also used for the determination of masses that are important
for the test of CVC, the unitary of the Cabibbo-Kobayashi-Maskawa (CKM)
matrix, and for putting constrains on the existence of scalars currents.
Measurements along this line include $^{74}$Rb (T$_{1/2}$=65 ms), which is
the shortest-lived nuclide studied in a Penning trap. The Q$_{EC}$ values of
$^{74}$Rb, determined with a precision of 6$\cdot $10$^{-8}$, serves as a
test of CVC or of related theoretical corrections [1]. Masses of $^{32}$Ar
and $^{33}$Ar have been determined with uncertainties of 6.0 $\cdot $
10$^{{\-}8}$ and 1.4 $\cdot $ 10$^{-8}$ [2]. The improved mass for $^{32}$Ar
helps to provide a better constraint on scalar contributions to the weak
interaction and both argon data serve as the most stringent test of isobaric
multiplet mass equation IMME. $^{34}$Ar, another CVC test candidate, has
been studied with an uncertainty of 1.1$\cdot $10$^{{\-}8}$ ($\delta $m =
0.41 keV). Similar precision has been achieved for $^{22}$Mg and neighboring
$^{21}$Na and $^{22}$Na [4]. The importance of these results is twofold:
First, an Ft value has been obtained for the super-allowed $\beta $ decay of
$^{22}$Mg to further test the CVC hypothesis. Second, the resonance energy
for the astrophysically relevant $^{21}$Na proton-capture reaction has been
independently determined.
[1] A. Kellerbauer et al., Phys. Rev. Lett. 93 (2004) 072502
[2] K. Blaum et al.,~Phys. Rev. Lett. 91 (2003) 260801
[3] F. Herfurth et al, Eur. Phys. J. A15 (2002) 17
[4] M. Mukherjee et al., Phys. Rev. Lett. 93 (2004) 150801
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2005.APR.X11.3