The annual AGATA collaboration meeting will be held at Legnaro National Laboratory on November 10-12, 2021, after the end of the Pre-PAC Workshop of AGATA@LNL (November 8-10).
The meeting will start in the afternoon of Wednesday, November 10th, with presentations on the status of the AGATA spectrometer at LNL and on the recent AGATA campaign at GANIL. Short presentations on recent results and on the status of ongoing analyses of AGATA experiments will be given on Wednesday 10th, Thursday 11th, and Friday 12th morning.
The yearly closed meeting of the AGATA Collaboration Council will take place on Thursday 11th, late afternoon.
According to the data policy agreement of the collaboration, status reports for the progress of the analysis of data obtained with AGATA must be given annually. Contact persons (or spokespersons) of AGATA experiments performed during the GANIL campaigns are requested to submit abstracts for short presentations at the annual AGATA collaboration meeting.
The deadline for abstract submission is 1st October 2021
Abstracts should be submitted through this page, with the title “Report on the AGATA@GANIL experiment Exxx”.
Attendees that would like to participate in person are kindly asked to check the current travel restriction imposed due to coronavirus pandemic. See COVID-19 status page.
For accommodation and traveling see Pre-PAC Workshop of AGATA@LNL web page.
In this work, we studied the structure of the pf-shell N=Z nucleus
[1] The AGATA Collaboration, Nuclear Instruments and Methods in Physics Research A, 668 (March) (2012), 26.
[2] C. Domingo-Pardo, et al. Nucl. Ins. and Meth. in Phys. Res. Sec. A 694 (2012) 297
[3] K. L. Yurkewicz, et al. Phys. Rev. C 70 (2004) 034301.
[4] K. Arnswald, et al. Physics Letters B 772 (2017) 599 – 606.
In order to shed light on the open question of the seniority conservation in the proton g9/2 orbital in the N=50 isotones [1,2], reduced transition probabilities in 90Zr, 92Mo and 94Ru nuclei, have been determined experimentally for the first time via lifetime measurements at the GANIL laboratory. The unconventional use of multi-nucleon transfer reaction [3] with a differential plunger device [4] allowed to measure lifetimes of the yrast low-spin states despite the presence of isomers in the proton-rich isotones. The required sensitivity to the lifetimes could only be achieved due to the excellent performance of the AGATA+VAMOS++ detection system [5,6].
The B(E2;4+->2+) and B(E2;2+->0+) yrast transitions in 92Mo and 94Ru and for the B(E2;4+->2+) and B(E2;6+->4+) yrast transitions in 90Zr determined in this experiment will be shown. In this contribution these results will be interpreted on the basis of realistic shell-model calculations [7] in the f5/2, p3/2, p1/2, g9/2 valence space, where it emerges that seniority is conserved in the first g9/2 orbital.
[1] P. Van Isacker, Phys. Rev. Lett. 100 (2008) 052501
[2] C. Qi, Phys. Lett. B 773 (2017) 616
[3] R. Broda et al. PLB 251 (90) 245
[4] A. Dewald et al., Prog. Part. Nucl. Phys. 67, 786 (2012)
[5] S. Akkoyun, et al., Nucl. Instr. and Methods in Phys. Res. A 668 (2012) 26
[6] M. Rejmund, et al., Nucl. Instr. and Methods in Phys. Res. A 646 (1) (2011) 184
[7] L. Coraggio et al., Phys. Rev. C 100 (2019) 014316 and references therein.
The experiment E708 was performed in GANIL in 2016, aiming to investigate evolution of collectivity in odd mass Ga isotopes around N=40 and neighbouring nuclei. The lifetime measurements of the low-lying states in nuclei of interest would allow us to deduce the transition probabilities and extend our knowledge of the interplay between single-particle and collective degrees of freedom in this mass region.
Low-lying states in
in deep-inelastic reaction in inverse kinematics with a
The experiment was performed with the AGATA tracking array coupled to the VAMOS++ spectrometer which allowed us to detect the gamma-rays in coincidence with recoils emitted in the
deep-inelastic reactions. Lifetime measurements were performed using the differential plunger device from University of Cologne and by applying the Recoil Distance Doppler Shift method.
The main physics goal, lifetime measurement of 5/2
Measured lifetime and deduced transition probabilities of the 5/2
measured by Coulomb excitation and plunger technique was investigated. Obtained results
are in agreement with those of previous plunger experiments. In addition, lifetimes of the low-lying states of germanium isotopes
Simulations of novae explosive nucleosynthesis predict the production of the radionuclide
An experiment was performed at GANIL facility to measure the lifetime of the key state at Ex = 7.786 MeV. The principle of the experiment is similar to the one used in [3]. With a beam energy of 4.6 MeV/u, the reaction
Preliminary results will be presented. Ejectiles, protons and
References
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[4] M. Friedman et al., Phys. Rev. C 101, 052802(R) (2020).
Some years ago, unnatural-parity doublet states in 212Po with spins of 4-, 6-, and 8-, which were observed to decay via strong E1 transitions to the yrast band in an experiment performed with the EUROBALL spectrometer, were interpreted as being of alpha-cluster structure. Subsequent theoretical work seemed to support this interpretation. The aim of experiment E693 was to study the alpha-cluster properties of the nucleus 212Po in more detail. Although the experiment was seriously hampered by target problems, its analysis still led to very important conclusions. The new experimental information, together with a detailled comparison with shell-model calculations, suggests that the states of interest have positive rather than negative parity and decay via strong M1 transitions.
Nuclei around N=60, Z=40 show a rapid variation in the deformation of their ground state with a rather small change in the neutron number. This feature manifests a subtle interplay between different aspects of the forces in the nucleus and makes this region an ideal testing ground for various nuclear structure theories. As an example, it is established that the ground state of Zr isotopes vary from nearly spherical for N<60 to well deformed after N=60 [1–4]. However, theoretical models do not agree on the shape evolution of Zr beyond N=60 [5–10].
Lifetime measurements in neutron rich isotopes are an effective way to shed light on the shape evolution in this region of the Segrè chart. For this purpose, a successful experiment was performed in 2017 at GANIL by using the AGATA array coupled to the VAMOS spectrometer. The fast timing array FATIMA and the Orsay Universal Plunger system was also installed, allowing lifetime measurements in the range of 1 ps to 1 ns. The data set obtained from this experiment contains hundreds of isotopes and is producing many new interesting results.
With this contribution we will present the actual status of the analysis of this experiment, with a brief overview of what as been already done, what is ongoing and which are the future expectations. The aim of the present analysis is to obtain reliable lifetime results and error estimations through a comprehensive application of the Differential Decay Curve Method for the measurement of the lifetime both in single gamma and in coincidence gamma-gamma. We will show preliminary lifetime results obtained after the improvement of the velocity resolution of the emitting nuclei from the VAMOS data.
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The goal of Experiment E706 was to measure lifetimes of excited states in neutron-rich fission fragments in the mass A≈110 region. A beam of 238U was incident on a 9Be target, which was mounted in the OUPS plunger device together with a Mg degrader foil. The fission fragments were identified in mass and atomic number in the VAMOS++ spectrometer, while γ rays were detected with the AGATA and FATIMA arrays. The data analysis from the experiment, which is proceeding at IJClab Orsay, CEA Saclay, and the University of Oslo, has so far resulted in a PhD thesis at Université Paris-Saclay [1]. The general overview of the experiment and results on even-even nuclei will be presented in the contribution of G.Pasqualato.
In this report, we will present the optimization of the analysis procedure to improve the mass resolution and identification of ions in VAMOS. An overview of the wide range of nuclides for which lifetimes are being extracted will be given, with a focus on odd-even nuclei. We will furthermore present new ideas on how to utilize the information on the ion velocity from a spectrometer for determining lifetimes with the recoil distance technique.
[1] S. Ansari, “Shape evolution in neutron-rich Zr, Mo and Ru isotopes around mass A=100”, PhD Thesis Université Paris-Saclay 2019
Light neutron-rich nuclei, such as C and N isotopes, are a fertile ground for nuclear structure and nuclear astrophysics studies. Several nuclei in this region were populated in an experiment realised in GANIL, employing the deep-inelastic reaction
This was the first experiment with NEDA and the full setup, and it suffered of some issues.
The (alpha+n) channel 63Ge has been searched carefully, so far without success. Many contaminating channels contribute to the background. In particular, we have found contaminant channels from the reaction induced by 40Ar, present in the beam producing residues with larger cross sections for neutron-evaporating channels. Oxygen contamination of the target is estimated to be 7% as well. Both contaminants, in the target and in the beam populate channel with higher cross section than 63Ge and therefore, so far it has not been possible to find its gamma lines. We remind that no gamma lines are known in this nucleus. In summary, the main goal of the experiment, 63Ge, is below the high background due to the contaminants in the beam and target.
However, some other channels are under analysis by students and researchers. In particular, we have found new transitions in the N=Z+1 65Ge and 64Ga.
The analysis of the angular distribution has been done for some channels. The analysis of the data from this experiment has been the subject of 3 bachelor thesis already finished and one in thesis is in progress. The lifetime of some states are being analysed in the framework of a PhD thesis.
The E703 experiment was performed at GANIL in April–May 2018, with the setup of AGATA-NEDA-DIAMANT. This measurement aimed at the observation of gamma rays emitted from excited states of the nuclei 102Sn and 103Sn, from which two-body neutron interactions, single-particle energies and N=Z=50 core excitations could be inferred. The data analysis is pursued in Warsaw, Stockholm and Uppsala.
In depth optimisation of conditions of AGATA-NEDA-DIAMANT event building, NEDA neutron-gamma discrimination, NEDA two-neutron discrimination, DIAMANT charged particle identification and of the timing of all the components of the system were done. Stability corrections and calibrations were also completed. Several replays of the entire data set were run, with various event-building time conditions, and multiplicity conditions of the three used detector systems. This was necessary in order to enable study of both delayed and prompt gamma-ray radiation, emitted from states below and above the 6+ isomeric state in102Sn (T½ = 400 ns).
These procedures resulted in a very clean identification of events in which the two known gamma rays of 102Sn, namely 497 and 1472 keV, were registered. The statistics of the identified events is very low, though. In the gamma-gamma coincidence spectrum gated on the 1472 keV line, obtained with the condition that 2 neutrons and 1 alpha particle are registered, as well as that the two gamma rays are registered within a 50 ns window, but could be delayed up to 2 μs with respect to the prompt RF signal, there are 15 counts in the 497 keV peak. The spectrum contains virtually no background.
The analysis of the data is continued, with the aim to identify new gamma-ray transitions emitted from excited states of 102Sn.
The study of the nuclear deformation for nuclei between
The experiment populated excited states in the mirror pair
In order to determine the lifetimes of the excited states, two different software packages have been used to perform Doppler Shift Attenuation Method analysis. Both methods have been tested in the
Shell evolution of neutron-deficient Xe isotopes:
Quadrupole and Octupole Collectivity above 100Sn
Status of the Analysis of the Experiment E730 performed with the
AGATA-NEDA-DIAMANT-OUPS set-up
M.L. Jurado-Gómez, IFIC, Spain E.Clément, GANIL, France, A.Gadea, IFIC, Spain J.J. Valiente-Dobón, INFN-LNL, Legnaro, Italy.
The region that lies just above the Z=50 closed shell in the vicinity of 100Sn exhibits original collective behaviors. With the development of collectivity when adding protons in the g7/2 shell, shape coexisting structures, strong octupole correlations and strong neutron-proton couplings arise. With this experiment, we aim to address specific aspects of the collectivity development when approaching the N=Z line in light Xe isotopes by performing a precise lifetime measurement of excited states in 112Xe. The quadrupole degree of freedom, relevant to investigate the neutron-proton correlations [1], will be investigated through the lifetime of the 2+ and 4+. Additionally the lifetime of the 5- state, possibly together with information on branching ratios, might help address the question of the enhancement of the octupole correlation in the neighborhood of 112Ba[2].
The experiment was performed at the AGATA-NEDA-DIAMANT setup installed at the GANIL laboratory, with the CSNSM “OUPS” plunger device [3]. The 112Xe nuclei was populated in a compound nucleus reaction with a 58Ni beam impinging on a 58Ni 1 mg/cm2 target in the 2 proton 2 neutron evaporation channel. A 197Au degrader with a thickness of 5 mg/cm2 was installed in the plunger device to degrade the reaction products energy without stopping them, in order to maximize the sensibility. The detection on at least a neutron in NEDA+Neutron Wall [4] in coincidence with a gamma-ray in AGATA [5,6] was used as trigger while the information of DIAMANT was used off-line for identification and selection of the particle emitting channels. Nine Target-Degrader distances, ranging from 22 to 1500 micrometers, have been used to determine the lifetimes of interest.
The calibration, alignment, definition of the neutrons and light charged particle conditions and final sorting of the data was completed before the end of 2019.
In this contribution, we will report on the on the status of the analysis and the preliminary findings.
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[2] G. de Angelis et al., Phys. Lett. B 535 (2002) 93.
[3] J.Ljungvall et al., Nucl. Inst. and Meth. A 679 (2012) 61.
[4] J.J. Valiente-Dobón et al., Nucl. Inst. and Meth. A 927 (2019) 81.
[5] A. Akkoyun et al., Nucl. Inst. and Meth. A 668 (2012) 26.
[6] E. Clément et al., Nucl. Inst. and Meth. A 855 (2017) 1.
Two recent measurements performed at GANIL studied the unbound nucleus
The unbound nucleus
This contribution will present our final results on the measurement of the one and two proton emission as well as the current status of the analysis of the gamma decay in an unbound nucleus.
We present new experimental results for a measurement utilising the combination of AGATA, MUGAST, and VAMOS for a determination of the astrophysical
An indirect
We will present the experimental set-up and analysis, results for the strongest populated resonances in
[1] M. R. Hall et al. Phys. Rev. C 99, 035805 (2019)
[2] R. H. Cyburt et al. Astrophys. J. 830, 55 (2016)
[3] J. Keegans et al. MNRAS, 485, Issue 1, Pages 620–639 (2019)
[4] M. Rejmund et al. NIMA 646, 184 (2011)
[5] S. Akkoyun et al. NIMA 668, 26 (2012)
[6] M. Assié et al. J. Phys.: Conf. Ser. 1643 012070 (2020)
[7] M. Assié et al. Submitted for publication in NIMA (2021)
The evolution of the nuclear shell closure along N=28 has gathered much interest due to the observed
discrepancies between the well established shell model with SDPF-U interaction and measurements of
the half-magic 46Ar isotope.
In particular, while remarkable agreement was observed between theoretical and experimental values
of Sn, transition probabilities measured with intermediate Coulomb excitation diverge by a factor of two
from their predicted values[1, 2]. The reason behind this mismatch has been pinned down to the proton
transition matrix elements[2] and hints at an incorrect description of the sd proton space below Z=20 [3].
The experiment we proposed aimed at shedding some light on this peculiar problem by directly
probing the proton component of the wavefunction via a proton-pickup direct reaction: 46Ar(3He, d)47K
at an energy of 350 MeV.
The experiment, performed at the Spiral 1 facility in GANIL with a post-accelerated radioactive 46Ar
beam impinging on a high-density cryogenic 3He target, will assess the amount of d3/2 state relative to
the s1/2 relying on a state-of-the-art experimental setup for a precise reconstruction of the kinematics of
the reaction.
The heavy reaction fragment was identi ed by the high acceptance magnetic spectrometer, VAMOS,
while the high-granularity silicon DSSSD detector, MUGAST, allowed the measurement of the angular
distribution of the light ejectile while also performing particle identi cation. The AGATA[5] gamma-ray
tracking germanium array measured the gamma rays produced by the decay of the 47K excited states.
Experimental results will be compared with theoretical models to infer information on the proton
wavefunction of 46Ar.
References
[1] A. Gade et al., Phys. Rev. C 74, 034322 (2006)
[2] S. Calinescu et al., Phys. Rev. C 93, 044333 (2016)
[3] Z. Meisel et al., Phys. Rev. Lett. 114, 022501 (2015)
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[5] S. Akkoyun et al., Nucl. Inst. Meth. A 668, 26-58 (2012)
Neutron-rich oxygen isotopes constitute a perfect playground for testing three-body forces.
For example, the neutron drip line is correctly predicted only when these forces are included in the calculation, as demonstrated by the work of Otsuka et al. [1].
In fact, standard shell model calculations including only two-body forces predict the drip line to be positioned at
The inclusion of three-body forces has the effect of raising the
The importance of three-body forces is now established, however their contribution has yet to be quantified.
For this purpose, the
The non-yrast states
Hence, electromagnetic properties of the
An experiment aimed at measuring the lifetime of these states was performed at GANIL (France).
The
The beam-like and target-like partners were detected using the VAMOS spectrometer [2] and the MUGAST array [3], respectively.
The chosen reaction and the MUGAST and VAMOS detectors guaranteed a strong control on the population of the excited states and the capability of eliminating the effect of the feeders.
The
The lifetimes of the states were measured using the Doppler-Shift Attenuation method by comparing the lineshape of the experimental peaks to realistic Monte Carlo simulations.
In this contribution, the lifetime of the
[1] T. Otsuka et al., Phys.\ Rev.\ Lett. 105, 032501 (2010).
[2] M. Rejmund et al., Nucl. Instr. and Meth. A 646, 184 (2011).
[3] M. Assiè et al., Nucl. Instr. and Meth. A, 1041, 165743 (2021).
[4] E. Clèment et al., Nucl. Instr. Meth. A 855, 1 (2017).