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A charge plunger device to measure the lifetimes of excited nuclear states where transitions are dominated by internal conversion

Authors :
Barber, L. (L.)
Heery, J. (J.)
Cullen, D. M. (D. M.)
Singh, B. S. (B. S. Nara)
Herzberg, R.-D. (R.-D.)
Müller-Gatermann, C. (C.)
Beeton, G. (G.)
Bowry, M. (M.)
Dewald, A. (A.)
Grahn, T. (T.)
Greenlees, P. T. (P. T.)
Illana, A. (A.)
Julin, R. (R.)
Juutinen, S. (S.)
Keatings, J. M. (J. M.)
Luoma, M. (M.)
O’Donnell, D. (D.)
Ojala, J. (J.)
Pakarinen, J. (J.)
Rahkila, P. (P.)
Ruotsalainen, P. (P.)
Sandzelius, M. (M.)
Sarén, J. (J.)
Sinclair, J. (J.)
Smith, J. F. (J. F.)
Sorri, J. (J.)
Spagnoletti, P. (P.)
Tann, H. (H.)
Uusitalo, J. (J.)
Vilhena, J. (J.)
Zimba, G. (G.)
Publication Year :
2020
Publisher :
Elsevier, 2020.

Abstract

A charge plunger device has been commissioned based on the DPUNS plunger (Taylor et al., 2013) using the in-flight mass separator MARA at the University of Jyväskylä. The ¹⁵²Sm(³²S,4n)¹⁸⁰ reaction was used to populate excited states in ¹⁸⁰. A lifetime measurement of the state \(2_1^+\) was performed by applying the charge plunger technique, which relies on the detection of the charge state-distribution of recoils rather than the detection of the emitted γ rays. This state was a good candidate to test the charge plunger technique as it has a known lifetime and depopulates through a converted transition that competes strongly with γ-ray emission. The lifetime of the \(2_1^+\) state was measured to be 480(10)ps, which is consistent with previously reported lifetimes that relied on the standard γ-ray techniques. The charge plunger technique is a complementary approach to lifetime measurements of excited states that depopulate through both γ-ray emission and internal conversion. In cases where it is not possible to detect Doppler-shifted γ rays, for example, in heavy nuclei where internal conversion dominates, it may well be the only feasible lifetime analysis approach.

Details

Language :
English
Database :
OpenAIRE
Accession number :
edsair.od......2423..100af95e6b5e8b067229610c8fd7abc0