Skip to main content
11–15 Jul 2022
Dubrovnik, Croatia
Europe/Zagreb timezone

Shape evolution in neutron-rich nuclei around mass 100: lifetime measurements in Zr isotopes

11 Jul 2022, 12:20
20m
IUC

IUC

Don Frana Bulića 4, Dubrovnik
Transitional nuclei and shape coexistence Transitional nuclei and shape coexistence

Speaker

Giorgia Pasqualato (INFN Sezione di Padova)

Description

Nuclei around N=60, Z=40 show a rapid variation in the deformation of their ground state with a rather small change in the neutron number. This feature manifests a subtle interplay between different aspects of the forces in the nucleus and makes this region an ideal testing ground for various nuclear structure theories. As an example, it is established that the ground state of Zr isotopes vary from nearly spherical for N<60 to well deformed after N=60 [1–4]. However, the drastic shape transition in Zr beyond N=60 is still a challenge for the description of different
theoretical models [5–11].

Lifetime measurements are an effective way to shed light on the shape evolution in this region of the Segrè chart. For this purpose, a successful experiment was performed in 2017 at GANIL by using the γ-ray tracking array AGATA [12] coupled to the magnetic spectrometer VAMOS [13]. The Orsay Universal Plunger system [14] was installed allowing lifetime measurements in the order of the picosecond with the Recoil Distance Doppler Shift technique [15]. The data set obtained from this experiment contains hundreds of isotopes and is producing many new lifetime results.

In this contribution I will present preliminary results for transition probabilities obtained for 98104Zr isotopes by applying the Differential Decay Curve Method of analysis [15], both in single gamma and in coincidence gamma-gamma.

REFERENCES
[1] Sven A.E. Johansson, Nuclear Physics 64, 147-160 (1965).
[2] E. Cheifetz, Phys. Rev. Lett. 25, 38-43 (1970).
[3] D.A. Arseniev, A. Sobiczewski and V.G. Soloviev, Nuclear Physics A 139, 269-276 (1969).
[4] R.K. Sheline, I. Ragnarsson and S.G. Nilsson, Physics Letters B 41, 115-121 (1972).
[5] P. Moller et al., Atomic Data and Nuclear Data Tables 59, 185-381 (1995).
[6] G.A. Lalazissis et al., Atomic Data and Nuclear Data Tables 71, 1-40 (1999).
[7] J. Skalski et al., Nuclear Physics A 617, 282-315 (1997).
[8] F. R. Xu et al., Phys. Rev. C 65, 021303 (2002).
[9] R. Rodríguez-Guzmán et al., Physics Letters B 691 202-207, (2010).
[10] J. Xiang et al., Nuclear Physics A 873, 1-16 (2012).
[11] T. Togashi et al., Phys. Rev. Lett. 117, 172502 (2016).
[12] S. Akkoyun et al., Nucl. Instr. Meth. in Physics Research A 668, 26 (2012).
[13] M. Rejmund et al., Nucl. Instr. and Meth. in Physics Research A 646, 184-191 (2011).
[14] J. Ljungvall et al., Nucl. Instr. Meth. in Physics Research A 679, 61-66 (2012).
[15] A. Dewald, O. Muller, P. Petkov, Prog. in Particle and Nuclear Physics 67, 786-839 (2012).

Authors

Andreas Goergen (University of Oslo (NO)) Giorgia Pasqualato (INFN Sezione di Padova) Joa Ljungvall (Université Paris-Saclay (FR)) Wolfram Korten (CEA Paris-Saclay)

Presentation materials