5–7 Dec 2018
CERN
Europe/Zurich timezone

Beta-delayed fission investigation of $^{188m1,m2}$Bi employing isomer-selective laser ionization

7 Dec 2018, 12:20
20m
503/1-001 - Council Chamber (CERN)

503/1-001 - Council Chamber

CERN

162
Show room on map

Speaker

Boris Andel (Comenius University in Bratislava (SK))

Description

A dedicated and world-wide unique program to study $\beta$-delayed fission ($\beta$DF) is being performed by our collaboration since a decade ago at the ISOLDE (CERN), e.g. [1,2,3]. In $\beta$DF, the mother nucleus undergoes $\beta$ decay to excited state in the daughter nucleus with the energy comparable to the fission barrier height and the daughter nucleus then fissions. The excitation energy is limited by $Q_\beta$ value of parent nucleus, which is usually below 10 MeV. Therefore, $\beta$DF represents so called low-energy fission, which is sensitive to structure of the nucleus. It allows us to investigate fission properties of exotic isotopes, for which other low-energy fission studies would be extremely difficult or currently impossible. For example, $\beta$DF measurements established a new region (and a new type) of asymmetric fission [1,2].

Beta delayed-fission of $^{188}$Bi was previously studied in JINR Dubna [4,5] and at SHIP, GSI Darmstadt [6]. There are two predominantly $\alpha$-decaying isomers in $^{188}$Bi with half-lives of 60 ms and 265 ms [7], and in these studies it was not possible to assign the fission to specific isomer, neither the total kinetic energy (TKE) nor fission fragment mass distribution measurements were done.

In this contribution, we report on the recent $\beta$DF measurement of $^{188}$Bi performed at ISOLDE. The key goal of our study was to investigate $\beta$DF properties of the isomers in $^{188}$Bi separately, and to attempt to probe the spin dependence of fission. To obtain isomerically-pure beams, we employed selective power of RILIS. Results of these investigations will be presented, including partial half-lives of $\beta$DF for each isomer, and TKE and fission fragment mass distribution for longer-lived isomer. Findings will be discussed in connection to partial half-lives systematics and theoretical calculation of fission fragment mass distribution.

REFERENCES
[1] A. N. Andreyev et al., Phys. Rev. Lett. 105, 252502 (2010).
[2] A. N. Andreyev, M. Huyse and P. Van Duppen, Rev. Mod. Phys. 85, 1541 (2013).
[3] L. Ghys et al., Phys. Rev. C 90, 041301(R) (2014).
[4] Yu. A. Lazarev et al., Inst. Phys. Conf. Ser 132, 739 (1993).
[5] Yu. A. Lazarev et al., Europhys. Lett. 4 , 893 (1987).
[6] J. F. W. Lane et al., Phys. Rev. C 87, 014318 (2013).
[7] A. N. Andreyev et al., Eur. Phys. J. A 18 , 39 (2003).

Author

Boris Andel (Comenius University in Bratislava (SK))

Co-author

Presentation materials

There are no materials yet.