https://doi.org/10.1140/epja/s10050-025-01509-5
Regular Article - Experimental Physics
Plasma-delay studies on heavy ion detection using PIPS at the LOHENGRIN recoil separator
1
Department of Physics and Astronomy, Uppsala University, Box 516, 751 20, Uppsala, Sweden
2
European Commission, Joint Research Centre (JRC), 2440, Geel, Belgium
3
Institut Laue-Langevin, 38042, Grenoble, France
4
Center for Exotic Nuclear Studies, Institute of Basic Science, (34126), Daejeon, Republic of Korea
5
University of Edinburgh, EH9 3FD, Edinburgh, UK
6
University of Manchester, M13 9PL, Manchester, UK
7
Extreme Light Infrastructure - Nuclear Physics (ELI-NP), Horia Hulubei National Institute for R&D in Physics and Nuclear Engineering (IFIN-HH), 077125, Bucharest-Magurele, Romania
a
ana.gomez@physics.uu.se
b
ali.al-adili@physics.uu.se
Received:
28
July
2024
Accepted:
9
February
2025
Published online:
15
March
2025
The VERDI fission spectrometer is designed to measure fragment velocities and kinetic energies to achieve high-precision yield measurements. It consists of two time-of-flight (TOF) sections, each hosting a micro-channel plate (MCP) and up to 32 passivated implanted planar silicon (PIPS) detectors. The main challenge to achieve accurate fragment velocities is the so-called plasma delay time (PDT) phenomena in the PIPS detectors. In this work, we present a dedicated experimental campaign at the LOHENGRIN fission-fragment recoil separator, to solve the pending PDT challenges. The PDT effect was systematically investigated, as a function of mass and energy, using a dedicated time-of-flight setup. In addition, the pulse height defect (PHD) was determined simultaneously. The studies were conducted for five PIPS detectors, in energies and mass numbers ranging from 20 to 110 MeV and A = 85 to 149, respectively. Using digital signal processing, an excellent timing resolution was achieved, reaching as low as 60 ps (one ) for the heavy ions. The PDT revealed a strong positive correlation with the ion energy and a weak negative correlation with the mass. The experimental PDT values determined from five detectors confirm a consistent systematic behavior with respect to mass and energy. Some systematic discrepancies were exhibited by two detectors, possibly due to the use of different pre-amplification chains. The PDT measurements ranged between 1 and 3.5 ns, for heavy ions relative to
-particles. The PHD values showed also a strong correlation with the ion energy, and moreover with the ion mass. The PHD for heavy ions was found to range between 2 and 8 MeV, relative to
-particles. Finally, a two-dimensional parameterisation was developed to model the experimental PDT data, as a function of mass and energy. This new model, which is valid in the fission fragment mass and energy regime, will be of benefit for heavy-ion velocity measurements, using silicon detectors, as done in VERDI.
The original online version of this article was revised: In this article the affiliation details for authors Yung Hee Kim and Ulli Köster were incorrectly given as ‘Present affiliation: Center for Exotic Nuclear Studies, Institute of Basic Science, Daejeon (34126), Republic of Korea’. Yung Hee Kim is affiliated to ‘Institut Laue-Langevin, 38042 Grenoble, France’ and ‘Present affiliation: Center for Exotic Nuclear Studies, Institute of Basic Science, Daejeon (34126), Republic of Korea’. Ulli Köster is affiliated to ‘Institut Laue-Langevin, 38042 Grenoble, France’.
An erratum to this article is available online at https://doi.org/10.1140/epja/s10050-025-01547-z.
© The Author(s) 2025
corrected publication 2025
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.