10TH International workshop on quantum phase transitions in nuclei and many-body systems

Manifestation of the Berry phase in the atomic nucleus 213Pb

13 Jul 2022, 10:10

20m

IUC

Symmetries of interacting boson and/or fermion systems Symmetries of interacting boson and/or fermion systems

Speaker

Jose Javier Valiente Dobon

Description

I will present some of our later results on the ${}^{213}$Pb neutron-rich nucleus [1] studied using the unique availability of a primary 1 GeV $A$ ${}^{238}$U beam and of the FRS-RISING setup at GSI. The products of the uranium fragmentation were separated in mass and atomic number and then implanted for isomer decay $\gamma$-ray spectroscopy. A level scheme from the decay of the $21/2^{+}$ isomer, based on $\gamma$ intensities, $\gamma$-$\gamma$ coincidences and state lifetimes was built up and the $E2$ transition probabilities from the $21/2^{+}$ isomer to two low-lying $17/2^{+}$ levels were also deduced.

This experimental data has evidenced one of the best examples of a semi-magic nucleus with a half-filled isolated single-j shell where seniority selection rules are obeyed to a very good approximation. In the most simple shell-model approach ${}^{213}$Pb can be described as five neutrons in the $1{\mathrm{g}}_{9/2}$ orbital on top of the ${}^{208}$Pb core. Large scale shell-model calculations in the full valence space beyond ${}^{208}$Pb confirm that although the $1{\mathrm{g}}_{9/2}$ orbital is not isolated in energy, it is found to carry the dominant component in the wave function of the low-energy states. The experimental level scheme and the reduced transition probabilities are in good agreement with the theoretical description that predicts the existence of two $17/2^{+}$ levels of a very different nature: one with seniority $\upsilon =3$, while the other with $\upsilon =5$. The absence of mixing between the two $17/2^{+}$ states follows from the self-conjugate character of ${}^{213}$Pb, where the particle-hole transformation defines an observable Berry phase that leads to the conservation of seniority for most but not all states in this nucleus.

The Berry phase [2], which is a gauge-invariant geometrical phase accumulated by the wavefunction along a closed path, is a class of observables that are not associated with any operator. It is a key feature in quantum-mechanical systems, that has far reaching consequences, and has been found in many fields of physics since its postulation in the eighties. In the atomic self-conjugate nucleus ${}^{213}$Pb, the quantized Berry phase is evidenced by the conservation of seniority under the particle-hole conjugation transformation. In atomic nuclei no experimental signature of the Berry phase was reported up to now.

[1] J.J. Valiente-Dob\’on et al., Physics Letters B 816, 136183 (2021).
[2] M. V. Berry, Proc. Roy. Soc. A392, 45 (1984).

Presentation materials

valiente_dobon_dubrovnik.ppt