25–30 May 2025
Daejeon Convention Center (DCC)
Asia/Seoul timezone

Emergence of different band structures in odd-odd Tl nuclei

Not scheduled
20m
Daejeon Convention Center (DCC)

Daejeon Convention Center (DCC)

Daejeon Convention Center, 107 Expo-ro, Yuseong-gu, Daejeon (4-19 Doryong-dong)
Contributed Poster Presentation Nuclear Structure Poster Session

Speaker

SNIGDHA PAL (Variable Energy Cyclotron Centre, Kolkata, India)

Description

Study of nuclei near proton shell closure $Z=82$ is important, as interplay between different shapes has been observed in this region. Recent experiments show triaxial shapes, in addition to the symmetric oblate shapes, in odd-odd Tl nuclei in A $\sim$ 190 region. The proton Fermi level for Tl lies near the $3s_{1/2}$ orbital, but highly shape driving $h_{9/2}$ and $i_{13/2}$ Nilsson orbitals intrude in this region at moderate deformation, the neutron Fermi level also lies near $i_{13/2}$ orbital, above $N=100$. The interplay of these orbitals is responsible to induce different shapes which are manifested in different band structures. The shape of Tl isotopes varies from near spherical in neutron rich $^{202,204}$Tl [1,2] to different deformed structures in neutron deficit Tl isotopes. Triaxial shapes in odd-A and odd-odd isotopes are manifested as Chiral and t-bands in $^{193,194,195,198}$Tl [3,4,5,6]. Magnetic Rotational (MR) bands were observed in $^{194,197}$Tl [7,8]. On the other hand, $^{189,191}$Tl have prolate-oblate shape coexistence [9,10]. However, not much is known for odd-odd $^{190,192}$Tl which seem to be the transitional ones between axial and non-axial shapes in Tl isotopes.
We have performed two experiments using $^{30}$Si and $^{16}$O beams from BARC-TIFR Pelletron LINAC facility and K-130 cyclotron at VECC in India, respectively, to study these nuclei by fusion-evaporation reaction. The INGA setup with up to 17 clover HPGe detectors were used to detect the prompt gamma rays. The level schemes of these nuclei are established and extended with confirmed J$^\pi$ assignments of the levels. The new results show the evidence of the presence of MR band and octupole correlation in these nuclei. Details will be presented in the conference.

References
[1] N. Fotiades, et al., Phys. Rev. C 76, 014302 (2007).
[2] N. Fotiades, et al., Phys. Rev. C 77, 024306 (2008).
[3] P. L. Mastieng et al., Eur. Phys. J. A 50: 119 (2014)
[4] T. Roy et al., Physics Letters B 782 768–772, (2018)
[5] E.A. Lawrie et al.,Eur. Phys. J. A 45, 39–50 (2010)
[6] J. Ndayishimye et al., Phys. Rev. C 100, 014313 (2019).
[7] H. Pai et al., Phys. Rev. C 85, 064313 (2012).
[8] S. Nandi et al., Phys. Rev. C 99, 054312 (2019).
[9] S. K. Chamoli, et al., Phys. Rev. C C 75, 054323 (2007).
[10] W. Reviol, et al., Physica Scripta. Vol. T56, 167-174, (1995).

Primary author

SNIGDHA PAL (Variable Energy Cyclotron Centre, Kolkata, India)

Co-authors

A. Karmakar (Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700064, India) A. Kundu (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) A. Pal (Variable Energy Cyclotron Centre, Kolkata, India) A. Sharma (UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India) A. T. Vazhappily (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) B. S. Naidu (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) Biswajit Das (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) C. Majumder (Indian Institute of Technology Bombay, Powai, Mumbai-400076, India) D. Kumar (Variable Energy Cyclotron Centre, Kolkata, India) Dr G. Mukherjee (Variable Energy Cyclotron Centre, Kolkata, India,) K. Banerjee (Variable Energy Cyclotron Centre, Kolkata, India,) P. Dey (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) P. Pant (Variable Energy Cyclotron Centre, Kolkata, India,) Pankaj K. Giri (UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India) R. Banik (Institute of Engineering and Management, Saltlake, Kolkata-700091, India) R. Kumar (Reactor Physics Design Division, Bhaba Atomic Research Center, Mumbai-85, India) R. Palit (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) R. Raut (UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India) R. Shil (Department of Physics, Visva-Bharati, Santiniketan-731235, India) Ms S. Basak (Variable Energy Cyclotron Centre, Kolkata, India) Mr S. Basu (Variable Energy Cyclotron Centre, Kolkata, India,) S. Bhattacharyya (Variable Energy Cyclotron Centre, Kolkata, India,) Dr S. Chakraborty (Variable Energy Cyclotron Centre, Kolkata, India) S. Das Gupta (Victoria Institution (College), Kolkata, India) S. K. Jadhav (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India) S. Kundu (UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India) S. Manna (Variable Energy Cyclotron Centre, Kolkata, India,) Dr S. Panwar (Variable Energy Cyclotron Centre, Kolkata, India) S. Rajbangshi (Department of Physics, Presidency University, Kolkata 700043, India) S. Roy (Variable Energy Cyclotron Centre, Kolkata, India) S. S. Ghugre (UGC-DAE CSR, Kolkata Centre, Kolkata 700098, India) Mr S. S. Nayak (Variable Energy Cyclotron Centre, Kolkata, India) Saumanti Sadhukhan (Variable Energy Cyclotron Centre, Kolkata, India) Dr Shabir Dar (Variable Energy Cyclotron Centre, Kolkata, India,) Dr Sneha Das (Variable Energy Cyclotron Centre, Kolkata, India) Dr Soumik Bhattacharya (Variable Energy Cyclotron Centre, Kolkata, India) Ms Suchorita Paul (Variable Energy Cyclotron Centre, Kolkata, India) Vishal Malik (Tata Institute of Fundamental Research, Homi Bhaba Road, Colaba, Mumbai-05, India)

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