- Bucher, B;
- Zhu, S;
- Wu, CY;
- Janssens, RVF;
- Cline, D;
- Hayes, AB;
- Albers, M;
- Ayangeakaa, AD;
- Butler, PA;
- Campbell, CM;
- Carpenter, MP;
- Chiara, CJ;
- Clark, JA;
- Crawford, HL;
- Cromaz, M;
- David, HM;
- Dickerson, C;
- Gregor, ET;
- Harker, J;
- Hoffman, CR;
- Kay, BP;
- Kondev, FG;
- Korichi, A;
- Lauritsen, T;
- Macchiavelli, AO;
- Pardo, RC;
- Richard, A;
- Riley, MA;
- Savard, G;
- Scheck, M;
- Seweryniak, D;
- Smith, MK;
- Vondrasek, R;
- Wiens, A
The neutron-rich nucleus ^{144}Ba (t_{1/2}=11.5 s) is expected to exhibit some of the strongest octupole correlations among nuclei with mass numbers A less than 200. Until now, indirect evidence for such strong correlations has been inferred from observations such as enhanced E1 transitions and interleaving positive- and negative-parity levels in the ground-state band. In this experiment, the octupole strength was measured directly by sub-barrier, multistep Coulomb excitation of a post-accelerated 650-MeV ^{144}Ba beam on a 1.0-mg/cm^{2} ^{208}Pb target. The measured value of the matrix element, ⟨3_{1}^{-}∥M(E3)∥0_{1}^{+}⟩=0.65(+17/-23) eb^{3/2}, corresponds to a reduced B(E3) transition probability of 48(+25/-34) W.u. This result represents an unambiguous determination of the octupole collectivity, is larger than any available theoretical prediction, and is consistent with octupole deformation.