D. Rosso

The TMR network project "Development of γ-ray tracking detectors"

The next generation of 4 pi arrays for high-precision gamma -ray spectroscopy will involve gamma -ray tracking detectors. They consist of high-fold segmented Ge detectors and a front-end electronics, based on new digital signal processing techniques, which allows to extract energy, timing and spatial information for a gamma -ray by pulse shape analysis of the Ge detector signals. Utilizing the information on the positions of the interaction points and the energies released at each point the tracks of the gamma -rays in a Ge shell can be reconstructed in three dimensions.

Gamma-ray tracking with the MARS detector

Abstract.The feasibility of the entire process of

Gamma-ray Tracking with Segmented HPGe Detectors

\gamma

Gamma‐ray Tracking With The MARS Detector

-ray tracking is demonstrated experimentally for the first time. The accuracy of the results is tested by the capability for Doppler correction of

Isospin character of low-lying pygmy dipole states in Pb 208 via inelastic scattering of O 17 ions

\gamma

Gamma-ray tracking arrays

-rays emitted in flight. The resolution of the 847.8 keV (

Light and heavy transfer products in Xe-136+U-238 multinucleon transfer reactions

2^ + \to 0^ +

In-beam experiment with the γ-ray tracking detector MARS

) transition detected with the MARS detector after Coulomb excitation of a 56Fe beam could be improved from 15 keV to below 5 keV (FWHM).

Isospin mixing in Zr 80: from finite to zero temperature

This paper gives a brief overview of the technical progress that can be achieved with the newly available segmented HPGe detectors. Gamma-ray tracking detectors are a new generation of HPGe detectors which are currently being developed to improve significantly the efficiency and resolving power of the 4 … germanium detectors arrays for high-precision ∞-ray spectroscopy. They consist of highly segmented HPGe detectors associated with fast digital front-end electronics. Through the pulse-shape analysis of the signals it is possible to extract the energy, timing and spatial information on the few interactions a ∞-ray undergoes in the HPGe detector. The tracks of the ∞-rays in the HPGe detector can then be reconstructed in three dimensions based on the Compton scattering formula. Such a detector has been used for the first time during an in-beam experiment. The ∞-decay of the Coulomb excitation of a 56 Fe nucleus was measured with the highly segmented MARS prototype positioned at 135 degree. The energy resolution has been improved by a factor of 3 as compared to standard HPGe detectors due to very precise Doppler correction based on knowledge of the ∞-ray track. I Introduction The future facilities for radioactive beams will allow, for the first time, the exploration of a new large area of the nuclear landscape. In connection with the study of the ∞-radiation, it is important to point out that the intensity of such radioactive beams is expected to be much smaller than that of stable beams, Doppler Effects in many experiments are expected to be much stronger and an intense background of X-rays could be present. Consequently, a new generation of powerful HPGe arrays with segmented detectors is being designed. Both in USA and in Europe several projects, based on segmented HPGe detectors, have already started and are in an advanced status of realization. The objective of the more recent R&D efforts is to improve the total efficiency by removing the BGO shields without affecting the P/T ratio with the use of the tracking technique, namely the reconstruction of the ∞-ray path to identify the ∞-incident direction (for the Doppler correction), the removal of the background and to check whether or not the ∞ was fully absorbed in the array. Such development implies unprecedented R&D efforts where completely new technology has to be applied, tested or developed in all the constituents of an HPGe array, from the detector to the front-end electronics. The typical feature of the energy deposition of a ∞-ray is that of interacting in a limited number of positions. ∞-tracking of this hits is a very challenging and ambitious task. First, one has to identify, isolate and localize each hit inside a segmented detector with pulse shape analysis based on the study of the physical mechanism of the pulse generation or with Artificial Intelligence techniques (like Neural Networks or Genetic Algorithm [1]) of the direct and induced electrical pulses produced by every interacting ∞-rays. Second, a tracking algorithm has to reconstruct the real trajectory from the list of interaction points through statistical techniques. The result is expected to be the complete reconstruction of the track of the incident ∞, namely the complete description of the interacting ∞-ray. Worldwide efforts have been done using simulations and proof-of-principle measurements and turned out to be successful. The feasibility of the entire process of ∞ray tracking is demonstrated in this paper based on an experiment, done at the LNL in Italy, using the MARS prototype detector.

Shape evolution in the neutron-rich osmium isotopes : Prompt gamma-ray spectroscopy of Os-196

The feasibility of the entire process of γ‐ray tracking is demonstrated experimentally for the first time. The accurracy of the results is verified by the capability to carry out Doppler correction of γ‐rays emitted in flight. The resolution of the 847.8 keV transition detected with the MARS detector after Coulomb excitation of a 56Fe beam could be improved from 15 keV to below 5 keV (FWHM).