TOPTIER CNS Summer School 2025
The TOPTIER CNS Summer School (TOPTIER-CNSSS25), hosted by Center for Nuclear Study, the University of Tokyo, will be held for Aug.22 - 28, 2025. The school has been held every summer since 2001 to foster the young generation of nuclear physics in Asia. The school is co-hosted by TOP-Tier platform In Extremely Rare isotope science project of Korea, Super Heavy Element Center (RCSHE), Center for Accelerator and Beam Applied Science (CABAS) of Kyushu University and Japan Physical Society. The school is also supported by ANPhA and RIKEN Nishina Center.
The venue of the school is the Conference hall of the RIKEN headquarter building in RIKEN wako campus (22, 25, 26, 27, 28th/Aug.) and Koshiba hall, Hongo campus, the University of Tokyo (23rd/Aug). The school aims to foster the young generation of nuclear physicists. The participants of the school will meet together to discuss the lectures in the relaxed atmosphere after each school day, which enhances the mutual understanding between participants.
The lecturers of the TOPTIER-CNSSS25 are,
- Prof. Dr. Calro Barbieri (Milano, It), "Ab initio methods for nuclear structure"
- Prof. Seonho Choi (SNU, KR), "Probing nuclear structure with electron beam (TBC)"
- Dr. Heather Crawford (LBL, USA), "In-beam gamma-ray spectroscopy in the era of GRETA (tentative)"
- Prof. Yasuko Kameyama (Sustainable Society Design Center, University of Tokyo), "Climate change and energy, International responses to climate change"
- Dr. Shin'Ichiro Michimasa (RNC), "Overview of RIBF and related topics"
- Prof. Taka Otsuka (Univ. of Tokyo), "Quantum many-body formulation of nuclear shapes, rotations, and vibrations"
- Prof. Taeksu Shin (IBS, KR), "Introduction of RAON and new opportunities"
- Prof. Ken'ichi Yoshida (RCNP, Univ. of Osaka), "Pairing and Superdeformation (tentative)"
As the past CNS Summer School, we will have young scientist sessions where the Ph.D students and Post-docs contribute to the oral presentation. From 2018 we select a few persons from the presentations as the winners of “CNSSS Young Scientist Awards”. The certificate will be given to the winners.
We plan to support the accommodation fee and travel expenses, although it is limited. The support will primarily come to those who perform an oral presentation. If you need the support, pls make the registration not later than Jul./22nd.
Regarding the fees for snacks and light meal during the poster session, we kindly ask that you contribute 1000 yen if you are a student, and 2000 yen if you are a postdoc or in another category.
We’re looking forward to seeing you at the school.
With best regards
TOPTIER-CNSSS25 Organizing Committee








-
-
1
Greetings
-
2
Ab initio methods for nuclear structure 1
-
10:50
break
-
3
Overview of RIBF and related topics (1/2)
-
11:55
Lunch
-
4
Beyond the Conventional: Hyperdeformation and Exotic Superfluidity in Atomic Nuclei (1/4)
-
14:20
brek
-
5
Overview of RIBF and related topics (2/2)
-
15:25
brak
-
RIBF facility tour
-
Welcome reception
Hirosawa club 2F
-
1
-
-
6
GreetingSpeaker: Prof. Shin'ichi Ohkoshi (School of Science)
-
7
Beyond the Conventional: Hyperdeformation and Exotic Superfluidity in Atomic Nuclei (2/4)
-
10:50
break
-
8
Ab initio methods for nuclear structure 2
-
11:55
Lunch break
-
9
Qantum many-body formulation of nuclear shapes, rotations, and vibrations (1/4)
-
14:20
break
-
10
Introduction of RAON and new opportunities
-
15:25
break
-
Young scientist session 1
-
11
Revised reaction rate for the astrophysical reaction 18O(p, α)15N via a global R-matrix analysis
The $\mathrm{^{18}O}(p, \alpha)\mathrm{^{15}N}$ reaction plays a crucial role in influencing the abundances of key isotopes such as $\mathrm{^{19}F}$, $\mathrm{^{18}O}$, and $\mathrm{^{15}N}$ in asymptotic giant branch (AGB) stars. This reaction may offer a potential mechanism to explain the discrepancies between observational data and theoretical model predictions.
A comprehensive $\mathit{R}$-matrix analysis of the $\mathrm{^{18}O}(p, \alpha)\mathrm{^{15}N}$ reaction has been conducted, incorporating supplementary constraints from other reaction channels, especially, the $\mathrm{^{15}N} + \alpha$ scattering data were involved in the analysis for the first time. All available experimental data have been systematically compiled and used in the $\mathit{R}$-matrix analysis.
A revised determination of reaction rate has been extracted relying on the present fitting parameters. The uncertainties on the corresponding reaction rates were then obtained by a Monte Carlo analysis. The currently determined reaction rates are systematically lower than those measured by Bruno $\textit{et al.}$ (2019), resulting in reduced depletion efficiency of $\mathrm{^{18}O}$ that consequently enhances its surface abundance in AGB stars. Therefore, this enables scientists to reduce reliance on dilution assumptions when interpreting observational data through theoretical models.
This work has been published in the Astrophysical Journal 973:93 (2024).Speaker: Mr Yiyang Li (Institute of Modern Physics, Chinese Academy of Sciences) -
12
Theoretical investigation of the production of superheavy nuclei near neutron closed and deformed shell regions
The existence of the island of stability has been predicted [1]. One of the major topics in nuclear physics is the production of $^{298}\mathrm{Fl}$, which is located at the center of this island.
A previous study [2] predicted that synthesizing a compound nucleus more neutron-rich than $^{298}\mathrm{Fl}$ (e.g. $^{304}\mathrm{Fl}$) may offer an advantage in terms of production probability. Firstly, due to its lower neutron binding energy, neutrons can be more easily evaporated. Furthermore, neutron emission brings the nucleus closer to the predicted neutron shell closure at $N = 184$, which increases the shell correction energy. These effects help to prevent a significant decrease in survival probability at high excitation energies.
In this study, these mechanisms are theoretically investigated using experimentally studied reaction systems. Particular attention is paid to $^{278}\mathrm{Ds}$ and $^{280}\mathrm{Ds}$ ($Z = 110$), formed via the $^{40}\mathrm{Ar}+^{238}\mathrm{U}$ and $^{48}\mathrm{Ca}+^{232}\mathrm{Th}$ reactions [3], respectively, near the deformed shell region at $N = 162$. We also discuss the synthesis of new elements in which these mechanisms may be confirmed.
We calculated the entire fusion-fission process in the superheavy region in three stages: (i) the projectile-target contact, (ii) the competition between fusion and quasi-fission, and (iii) the decay of the excited compound nucleus. We employed the coupled-channel method [4, 5] for stage (i), the multidimensional Langevin approach [5] for stage (ii), and the statistical model [6] for stage (iii).
In this presentation, we primarily discuss the effect of neutron evaporation and the resulting increase in the shell correction energy. This effect plays a crucial role in the survival probability of the compound nucleus. It may also play an important role in reaching the island of stability.References
[1] W. D. Myers and W. J. Swiatecki, Nucl. Phys. 81, 1 (1966).
[2] Y. Aritomo, Phys. Rev. C 75, 024602 (2007).
[3] Yu. Ts. Oganessian, et al., Phys. Rev. C 109, 054307 (2024).
[4] K. Hagino, et al., Computer Physics Communications 123 (1999) 143–152.
[5] Y. Aritomo, et al., Phys. Rev. C 85, 044614 (2012).
[6] M. Ohta, Proceedings of Fusion Dynamics at the Extremes, pp. 110-122 (2001).Speaker: Kosuke Kawai (Kindai University) -
13
The multimodality of Ir-187 fission
As a complex, large-amplitude deformation quantum many-body system, nuclear fission reflects the competition between single-particle and collective behaviors, leading to the coexistence of multiple fission modes for the same fissioning nucleus. Both past and recent experiments indicate that $^{187}$Ir undergoes predominantly symmetric fission, while several theoretical predictions favored asymmetric fission. In this presentation, I will report our analysis of the fission modes of $^{187}$Ir and discuss possible reasons for the dominance of symmetric fission.
Speaker: Mr Yingge HUANG (Sun Yat-sen Univ. / Univ. of Tokyo) -
14
Microscopic Study of 10C: 2α + 2p Clustering Structure and Diproton Correlations
We investigate the cluster structure of $^{10}\mathrm{C}$ using a microscopic four-body $\alpha + \alpha + p + p$ cluster model within the Generator Coordinate Method (GCM) framework. The calculated low-lying energy spectrum is in good agreement with the experimental data. Based on the analysis of reduced width amplitudes (RWA) and spectroscopic factors (SF) for the two-body decay channels ($^{9}\mathrm{B} + p$, $^{6}\mathrm{Be} + \alpha$, and $^{8}\mathrm{Be} + 2p$), as well as the three-body clustering configuration ($^{8}\mathrm{Be} + p + p$), several developed cluster structures are identified. The analysis reveals that the $0_1^+$ state corresponds to a compact structure, while the $0_2^+$ and $2_3^+$ states show significant diproton clustering components. In particular, the $0_2^+$ state is found to exhibit a mixed structure, characterized by both pronounced $\alpha$-clustering and diproton configurations, consistent with previous theoretical predictions and experimental observations. It is also found that the $2_1^+$ and $2_2^+$ states predominantly indicate shell-model-like characteristics, while the $0_3^+$ state displays a more spatially extended configuration.
Speaker: Liudi Song (Fudan university) -
15
Probing shell structure at N=32 and 34 far from stability with realistic nuclear forces
The nuclei, characterized by large $N/Z$ ratios, are often referred to as exotic nuclei and challenge the traditional understanding of nuclear shell structure. The conventional magic numbers, such as $N=$8, 20, 28, etc., tend to diminish or vanish, and new magic numbers emerge in the exotic systems. In this work, we investigated the appearance of new magic numbers at $N=32$ and 34 and their evolution in neutron-rich isotopes lying above and below Ca. We studied the shell gaps from the underlying two- and three-nucleon forces obtained from QCD-based chiral effective field theory, employing the state-of-the-art ab initio valence-space in-medium similarity renormalization group method. The development of shell gaps at $N=32$ and 34 is discussed from various nuclear observables and effective single-particle energies. Our calculated results align well with the available experimental data and suggest a strengthening of the $N=34$ sub-shell gap while the $N=32$ sub-shell gap weakens or disappears below Ca. To understand the microscopic origin of these shell effects, we analyzed different components of the nuclear interaction -central, spin-orbit, and tensor- through spin-tensor decomposition and elucidated their roles in establishing shell gaps far from stability. Then, the low-energy structures of the exotic $N=32$ isotones, adjacent to the $N=34$ shell gap, are studied in detail. It is observed that these nuclei exhibit deformed ground states and coexist with a weakly deformed band at low-excitation energy. The present work demonstrates essential components of nuclear force in shaping magic numbers far from stability and offers deeper insights into the structure of exotic nuclei from the underlying nucleon-nucleon interactions.
Speaker: Subhrajit Sahoo (Indian Institue of Technology Roorkee) -
16
The candidates of 2alpha condensate around the oxygen16 nucleus studied by the Real-time evolution method
Nowadays, searching for $\alpha$ condensation around a core nucleus is an interesting topic. Previous theoretical studies predicted $^{16}$O+2$\alpha$ condensed states. However, there was strong mixing with non-resonant states and it causes the identification of true resonant states non-trivial.
To address this issue, we aim to provide a more robust theoretical verification of the $^{16}$O+2$\alpha$ condensation to identify the resonant states and predict their properties.
We employ the real-time evolution method(REM), which generates physically important basis states using the equation of motion, minimizing contamination from the continuum. The analytical continuation in the coupling constant (ACCC) was used to estimate the $\alpha$-decay widths.
The present results point out much better convergence of eigenstates, and the 0$^{+}_3$ and 0$^{+}_4$ states showed remarkable isoscalar monopole transition strengths, which were in good agreement with the previous theoretical work. The small $\alpha$-decay widths for these states suggest that experimental observation appears feasible.
Therefore, The real-time evolution method (REM) proved effective in identifying the candidates of 2$\alpha$ condensate around the $^{16}$O nucleus.Speaker: Ms Ya Min Htet (Faculty of Science, Hokkaido University) -
17
Beta Decay Study Using Shell Model
Beta decay is one of the fundamental weak interaction processes in nuclear physics that is crucial in shaping our understanding of nuclear structure. It also provides important insights into various astrophysical phenomena like r−process which is responsible for forming about half of the heavy elements in the universe beyond iron [1]. In this talk, I will discuss the beta decay properties which includes Fermi and Gamow Teller transitions, phase-space factor, log$ft$ and half-life. These concepts help to explain which transitions are allowed, how strong they are and how likely they occur. They are also essential for calculating decay rates and comparing theoretical predictions with experimental data. Studying nuclei in the lighter mass region with Z= 8−15 are particularly important because these nuclei are relatively simple, well understood, making them ideal for testing nuclear models like the shell model [2]. Our work focuses on studying the allowed beta decay properties in sd-shell nuclei, such as Gamow Teller matrix elements, their transition strengths (B(GT )), log$ft$ values, and branching ratios..etc. Our preliminary results obtained for several transitions like $^{21}\text{O} \rightarrow ^{21}$F, $^{21}\text{F} \rightarrow ^{21}$Ne and $^{24}\text{Ne} \rightarrow ^{24}$Na are in good agreement with available experimental data. We aim to address these fundamental properties in nuclei that are of current experimental interest and relevant to astrophysical nucleosynthesis processes.
References
[1] I. N. Borzov, “Beta-decay rates", Nucl. Phys. A 777, 645 (2006).
[2] A. Kumar, P. C. Srivastava, and T. Suzuki, “Shell model results for nuclear β−-decay properties of sd-shell nuclei, "Prog. Theor. Exp. Phys. 2020, 033D01 (2020).Speaker: Ms Nidhi Pant (Research Scholar, Department of Physics, IIT Roorkee, India) -
18
Probing the shell structure and interplay of configuration in neutron-rich N=50 nuclei
Exploring the nuclear shell structure of neutron-rich N = 50 nuclei is one of the most interesting and mysterious phenomena in nuclear physics, and it has become the forefront of both experimental and theoretical research in recent years. We have constructed the shell model Hamiltonian in the π(f p)-ν(sdg) model space based on an ab initio approach using VS-IMSRG(3f2) with minimal phenomenological adjustments to the single-particle energies to reproduce the recently available experimental data in the N = 50 region. To perform the large-scale shell model calculations, we have carried out the state-of-the-art
advanced Monte-Carlo Shell Model (MCSM) to interpret the nuclear structure properties of nuclei near the neutron magic number N = 50. Our MCSM-calculated nuclear structure properties, based on the new shell model Hamiltonian derived from VS-IMSRG(3f2), show a rather good qualitative agreement with the experimental data and previous shell model predictions. The prediction of structural properties in the N = 50
The region has significant implications for nuclear astrophysics, as it affects nucleosynthesis pathways and contributes to the distribution of elemental abundances in the universe.Speaker: ANIL KUMAR (Center for Computational Sciences, University of Tsukuba, Tsukuba, Japan) -
19
Harmonic oscillator model analysis of nuclear radius and neutron skin thickness
improve the harmonic oscillator model and test its performance for nuclear charge radii and neutron skin thicknesses
Speaker: Seong Yeon Kim (Soongsil University) -
20
Mass Prediction of Neutron-Deficient Fe, Ni, Zn, and Kr Isotopes Based on Mirror Energy Differences
Recent $B\rho$-defined isochronous mass spectrometry experiments have determined the masses of proton-rich nuclei such as $^{23}$Si, $^{26}$P, $^{27}$S, and $^{31}$Ar. These results confirm the bound nature of these isotopes and establish the location of the proton dripline for several isotopic chains. Notably, the measured mirror energy differences (MEDs) exhibit clear deviations from mirror symmetry in P, S, and Ar isotopes, suggesting the presence of extended proton distributions.
Based on these findings, we conducted a systematic theoretical study of MEDs across mirror nuclei, revealing a smooth quadratic dependence on the neutron–proton asymmetry $(N-Z)$. Utilizing this regularity, we made high-precision mass predictions for a series of neutron-deficient nuclei. Furthermore, the predicted masses are consistent with the Isobaric Multiplet Mass Equation (IMME), and the cubic term is found to be negligible, reinforcing the validity of isospin symmetry in this region.
Speaker: YUE YU (Institude of Modern Physics, Chinese Academy of Science)
-
11
-
6
-
-
homework
-
-
-
21
in-beam gamma-ray spectroscopy in the era of GRETA (tentative) (1/4)
-
10:50
break
-
22
Climate change and energy
-
11:55
Lunch
-
23
Ab initio methods for nuclear structure 3
-
14:20
break
-
24
Beyond the Conventional: Hyperdeformation and Exotic Superfluidity in Atomic Nuclei (3/4)
-
15:25
break
-
Young Scientist Session 2
-
25
Progress on AMS Measurement of 60Fe in the Chang'E-5 lunar soil sample
The Moon provides a unique environment for investigating nearby astrophysical events such as supernovae. Lunar samples retain valuable information from these events, via detectable long-lived "fingerprint" radionuclides such as $^{60}$Fe. We are developing the accelerator mass spectrometry (AMS) method for detecting $^{60}$Fe using the HI-13 tandem accelerator at the China Institute of Atomic Energy. For our experiments, We have been allocated 200 mg of Chang'E-5 lunar soil samples by the China National Space Administration.
The identification of $^{60}$Fe with AMS is highly challenging due to strong isobaric interferences. Such interferences could not be sufficiently suppressed by the existing magnetic systems of the HI-13 tandem accelerator and the following Q3D magnetic spectrograph. To lower the detection background for the low abundance nuclide, a Wien filter was installed after the accelerator magnetic systems. A 1 μm thick ${\text{Si}_3\text{N}_4}$ foil was installed in front of the Q3D as an energy degrader. For particle detection, a multi-anode gas ionization chamber was mounted at the center of the focal plane of the spectrograph. An $^{60}$Fe standard sample with an abundance of $1.125 \times10^{-10}$ was used to test the new AMS system. These results indicate that $^{60}$Fe can be clearly distinguished from its isobar. In this presentation, we will report the current status of this experiment.
Speaker: zhang yang -
26
β-decay spectroscopy of proton-rich nucleus 28S
As member of the Tz=-2 family, 28S is a nucleus rather light near the proton drop line, and has high β-delayed proton (βp) branching ratio. Precise β-decay spectroscopy of proton-rich nucleus 28S serves as a powerful tool to study the isospin symmetry breaking, and to test the unitarity of CKM matrix through the superallowed Fermi transition between isobaric analog states. Nevertheless, only one experimental study was previously published by Pougheon et al. without detecting γ rays in 1989. The present work was conducted at Heavy Ion National Laboratory of Accelerator (HIRFL) in Lanzhou. The interested nucleus 28S was produced through projectile fragmentation (PF) method where 32S16+ beam (about 80 MeV/u) bombarded 9Be target, and subsequently implanted in a detector system composed of double-sided silicon strip detectors (DSSD), quadrant silicon detectors (QSD), and clover-type high-purity germanium detectors. Based on this detector system, our team has achieved excellent results for 22Si, 26Si, 26P, and 27S in recent years.
By measuring p and γ following β decay, the half-life and energy with higher accuracy were obtained. Different decay channels were clearly identified through the coincidence method to construct complete decay scheme, and the results were consistent with theoretical calculations. The mirror nuclei 28S-28Mg was also studied, which gave no evidence for existence of isospin symmetry breaking.Speaker: YUFENG GAO (Institute of Modern Physics, Chinese Academy of Sciences) -
27
Latest Achievement on the UCN source of the TRIUMF Ultracold Neutron and the EDM Experiment
A non-zero electric dipole moment of the neutron (nEDM) would violate the CP symmetry and be related to baryon asymmetry in our universe. The TRIUMF Ultracold Advanced Neutron (TUCAN) collaboration is commissioning a world-leading ultracold neutron (UCN) source for such precise measurements of the nEDM. With such an intensive UCN source, the TUCAN collaboration aims to push the statistical nEDM measurement sensitivity to the scale of $10^{-27}$ e$\cdot$cm within 400 days. Spallation neutrons will be cooled with room temperature heavy water and 20K liquid deuterium, after which, the UCNs will be produced in a spherical volume in 1K superfluid helium. These UCNs are then extracted from the production volume and introduced to the experimental equipment with coated vacuum neutron guides. Once the source is completed, it will provide a UCN production rate of $1.6\times10^7$/s.
The UCNs produced from the source will be transferred to the storage unit, and the nEDM will be measured later by the Ramsey resonance technique with separated oscillating magnetic fields. This source can also be applied to other experimental proposals, such as neutron lifetime measurement or the search for axion-like particles. This presentation will focus on the latest achievement on the UCN source commissioning and the nEDM experiment at TRIUMF, including initial UCN production results from operating the superfluid He-II source prior to installation of the LD2 moderator.
Speaker: Kelin Qiao (on Behalf of the TUCAN Collaboration) (The University of Osaka / Research Center for Nuclear Physics (RCNP)) -
28
Octuple Correlation in 67Ga
High-spin states of $^{67}$Ga have been studied via the $^{58}$Ni($^{12}$C, 3p)$^{67}$Ga fusion-evaporation reaction at a beam energy of 50.4 MeV. Three negative-parity bands and three positive-parity bands in $^{67}$Ga are established. The observation of one new $E3$ transition linking the positive-parity $\pi 1g_{9/2}$ band and negative-parity $\pi 2p_{3/2}$ band provides evidence of octuple correlations in $^{67}$Ga. The characteristics of octuple correlations in the $^{67}$Ga are discussed in terms of the reflection-asymmetric triaxial partical rotor model and microscopic relativistic mean field+Bardeen-Cooper-Schrieffer model.
Speaker: Jiayi Yi (School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University) -
29
Proton elastic scattering from 50Ca at the RIKEN RIBF toward future studies of the nuclear matter EoS
Constraining the equation of state (EoS) of nuclear matter remains one of the key open questions in both nuclear physics and astrophysics, with significant implications for phenomena such as neutron stars and supernova explosions. One approach is to investigate the differences in proton and neutron density distributions across isotopic chains, which are expected to provide a valuable insight into the symmetry energy of the nuclear matter EoS. Proton elastic scattering is known to be highly sensitive to the neutron and proton density distributions, particularly in magic nuclei such as calcium ($Z=20$) and tin ($Z=50$), where the closed proton shells enhance this sensitivity.
A measurement of proton elastic scattering for the neutron-rich nucleus $^{50}$Ca has been performed in inverse kinematics at the RIKEN RI Beam Factory (RIBF). The experiment employed a newly developed $∆E-E$ telescope array, DELTA, consisting of Silicon Strip Detectors (SSD) and GAGG(Ce) calorimeters, to reconstruct the four-momentum of recoil protons. In this presentation, we report the results of the $^{50}$Ca($p,p$) elastic scattering experiment, focusing on the extracted angular distributions. We also outline future plans to extend this study to rare isotopes $^{52}$Ca and $^{104}$Sn and present ongoing developments toward the next experimental campaign.Speaker: Tomoya Nakada (Kyoto University) -
30
Development of $^{10,11}$B Targets and Data Acquisition Systems for the Measurement of the $^{10,11}$B($^3$He,$t$)$^{10,11}$C Reactions
Big Bang Nucleosynthesis (BBN) refers to the nuclear reactions that occurred approximately from 10 seconds to 20 minutes after the birth of the universe. These reactions produced light elements, mainly $^2$H, $^3$He, $^4$He, and $^7$Li. The standard BBN model reproduces the abundances of these elements with high precision, except for $^7$Li. This agreement is regarded as strong evidence that the universe was once in a hot and dense state in the early phase of its evolution. However, BBN has an unresolved major issue known as the ``cosmological lithium problem.'' The abundance of $^7$Li calculated by BBN is approximately three times higher than the value inferred from astronomical observations. This discrepancy remains a serious challenge in modern physics.
Our research aims to address this $^7$Li problem from the perspective of a nuclear experiment. $^7$Li was produced primarily through the electron capture decay of $^7$Be, which was synthesized during BBN. Many studies have already investigated the production of $^7$Be, and there is little room to significantly alter its abundance in standard BBN calculations.
We investigate the possibility that $^7$Be is transformed into nuclei other than $^7$Li through unknown reaction channels before it undergoes electron capture. Theoretical studies have proposed that unknown resonant states exist in $^{10}$C and $^{11}$C. These nuclei are formed through the $^7$Be + $^3$He and $^7$Be + $^4$He reactions, respectively. If such resonant states exist and allow the conversion of $^7$Be into other nuclei via these resonances, the final abundance of $^7$Li in BBN would decrease.
We plan to measure the ($^3$He,$t$) reactions on $^{10}$B and $^{11}$B to search for these resonant states. The $^7$Be + $^3$He and $^7$Be + $^4$He resonances are expected to appear at excitation energies of 14.9–15.2 MeV in $^{10}$C and 7.79–7.90 MeV in $^{11}$C, respectively. Therefore, we will conduct high-resolution measurements using the Grand Raiden (GR) spectrometer at RCNP. In addition to detecting tritons with GR, we will also identify the decay particles from the excited states of $^{10}$C and $^{11}$C using Si detectors.
To conduct this experiment, we have carried out two technological developments. First, in collaboration with MicroMatter Technologies in Canada, we fabricated a self-supporting $^{11}$B thin film target using pulsed laser deposition. The impurity content of this target was evaluated through the $^{10,11}$B($d$,$p$) reaction, which revealed approximately 8$\%$ contamination from $^{12}$C. We are also planning to develop a $^{10}$B target in July and to evaluate its impurity content using the same method. The results will be presented in this poster.
Second, we addressed the challenge of identifying coincident events between GR and Si detectors. The GR system is based on a trigger-less streaming DAQ, whereas the Si detectors use a trigger-based DAQ system. Since these two systems employ different data acquisition methods, reconstructing events between them required a creative approach. We solved this issue by reading the accepted trigger signal from the Si detectors with the GR system.
This poster presents the development of thin film targets, impurity evaluation results, and the integration of DAQ systems between GR and silicon detectors.
Speaker: 奨太朗 前里 (大阪大学) -
31
Direct measurement of the carbon-carbon fusion cross section at stellar energies
The carbon-carbon fusion reaction serves as a crucial reaction for stellar evolution and explosive events, significantly influencing the evolution of massive stars and the explosion of superburst in the Universe. Despite decades of research, there remains considerable uncertainty in the cross section, particularly at stellar energies below E_{C.M.}=3MeV. The extrapolation techniques cannot provide a clear picture of the reaction within the Gamow window. We measured the cross section of ^{12}C(^{12}C,a_{0})^{20}Ne in the energy range of E_{C.M.}=2.3 MeV to 3.6 MeV using an intense carbon beam with intensity up to 100 particle microamperes, provided by the LEAF accelerator in Lanzhou, and a novel detection system comprising a time projection chamber (TPC) and a silicon detector array. Our direct measurement results yield new values for the reaction cross section, indicating that further improvements are needed in the THM indirect method. A new reaction rate is recommended based on our experimental result.
Speaker: Yunzhen Li (Institute of Modern Physics) -
32
Resonance of K*0(892) in and out of jets in pp collisions at sqrt(s) = 13.6 TeV
Recent measurements of two-particle correlations within jets in high-multiplicity pp collisions at √s = 13.6 TeV reveal flow-like patterns among jet constituents. Such effects were previously considered unique to heavy-ion collisions, suggesting that a hot, dense QCD medium may form even inside jets in small systems. As this medium hadronizes, substantial final-state hadronic interactions can persist, leading to significant modifications of short-lived resonance yields through (pseudo-)elastic scatterings with other hadrons after chemical freeze-out. To investigate this, we analyze yields of the short-lived K⁰ meson using high-multiplicity jets in pp collision data at √s = 13.6 TeV collected by the ALICE Collaboration during LHC Run 3. Charged-particle jets are reconstructed, and per-jet K⁰ yields are measured in and out of the jet cone. Comparing these yields for this resonance offers new insight into final-state hadronic interactions inside jets produced in small collision systems.
Speaker: Jimun Lee (Sejong University)
-
25
-
21
-
-
33
in-beam gamma-ray spectroscopy in the era of GRETA (tentative) (2/4)
-
10:50
break
-
34
Beyond the Conventional: Hyperdeformation and Exotic Superfluidity in Atomic Nuclei (4/4)
-
11:55
Lunch
-
35
Quantum many-body formulation of nuclear shapes, rotations, and vibrations (2/4)
-
14:20
break
-
36
International responses to climate change
-
15:25
break
-
Young Scientist Session 3
-
37
Implication of neutron star observations to the origin of nucleon mass
We investigate the implications of neutron star observations for understanding the origin of nucleon mass using a framework that combines three complementary approaches: the parity doublet model for hadronic matter below 2n0, the Nambu-Jona-Lasinio (NJL) model for quark matter above 5n0, and a model-independent analysis of the intermediate density region based on fundamental physical principles. By systematically exploring parameter spaces and comparing theoretical predictions with recent observational constraints, we establish constraints on the chiral invariant mass in the PDM. Our results suggest that more than a half of the nucleon mass originates from sources beyond spontaneous chiral symmetry breaking, challenging conventional understanding of nucleon mass generation. These constraints arise solely from fundamental physical principles and observational data, independent of specific assumptions about the nature of the quark-hadron transition, providing robust insights into the microscopic origin of hadron masses.
Speaker: Xiang LIU (Nagoya University) -
38
Interplay Between 3P2 Neutron Quantum Vortices and 1S0 Proton Fluxtubes in the Outer Core of Neutron Stars
Neutron stars exhibit sudden changes of its rotational velocity, known as "pulsar glitches". It has been believed that glitches are mainly caused by superfluid neutron vortices in the inner crust of neutron stars. However, importance of contributions of the outer core has been recently discussed, and further microscopic investigations of quantum vortices and fluxtubes in the outer core of neutron stars are highly desired.
In this study, we investigate the interaction between quantum vortices of $^3P_2$ superfluid neutrons and fluxtubes of $^1S_0$ superconducting protons in the outer core of neutron stars, based on a successful bosonic theory of superfluid, the Gross-Pitaevskii equation (GPE). In this talk, we will discuss how the $^3P_2$ superfluid vortices interact with proton fluxtubes under a magnetic field in the outer core of neutron star.Speaker: Tatsuhiro Hattori (Institute of Science Tokyo) -
39
Sensitivity study of Neutrino opacities to Skyrme EOS in CCSNe
When a core-collapse supernova (CCSN) explodes, it emits an enormous number of neutrinos, which carry away approximately 99% of the total energy.
These energetic neutrinos play a crucial role in both the explosion mechanism and nucleosynthesis as they propagate through the CCSN environment.
The propagation of neutrinos can be described by the general relativistic Boltzmann equation, in which the collision can affected by term equation of state .
In the equation of state, there are nonrelativistic models based on Skyrme interactions and relativistic models using relativistic mean field (RMF) theory.
Such modifications can alter neutrino opacities and transport properties, potentially affecting the supernova explosion and neutrino process.
We present a comparative study quantifying the sensitivity of neutrino interaction rates to representative Skyrme and RMF EOSs and discuss the resulting implications for neutrino luminosity predictions in CCSN.Speaker: Young_so Choi (Soongsil University) -
40
Real-time monitoring nuclear motion using high-order harmonic generation
Nuclear motion in molecules can be monitored in real time by using the combination of two laser pulses, one for initializing the interest dynamics and one for exciting the molecule to emiss the high-frequency photons, which is also known as high-order harmonic generation (HHG). In this work, we study the possibility of using HHG to monitor the movement of hydrogen nucleus in the dissociative process of H2 molecule and isomerization of HCN/HNC. Within adiabtic approximation, the nuclear and electronic motions are treated separately and simulated by solving the time-dependent Schrodinger equation. The results show the significant changes in HHG spectra versus the movement of H nucleus in the interest processes, proving for the possibility of using HHG to monitor molecular dynamics in real time. The project is still ongoing.
Speaker: An Trieu (Institute of Fundamental and Applied Sciences, Duy Tan Univeristy, Vietnam) -
41
ab initio effective operator study dripline nuclei observables
Recent studies of nuclei near driplines have signifcantly enhanced our understanding of nuclear structure. In those nuclei, the continuum coupling is crucial in reproducing weakly bound and unbound phenomena. To study the observables of the nuclei as open quantum systems self-consistently, we developed valence-space efective operators in the Berggren basis using many-body perturbation theory[1]. The two- plus three-nucleon force from the chiral efective feld theory has been used.
The observed β-decay isospin asymmetry between the dripline nucleus $^{22}$Si and its mirror partner $^{22}$O is reproduced, highlighting the crucial role of the $s_{1/2}$ continuum. Additionally, continuum efects also play a pivotal role in the signifcant Tomas-Ehrman shift observed between the mirror daughters $^{22}$Al and $^{22}$F[1].
Recent measurements of the E2 transition rate from the ground state to the frst $2^+$ excited state of the proton dripline nucleus $^{36}$Ca show an unusual patern when compared to its isotopic neighbor $^{38}$Ca: despite having a higher $E(2^+_1)$ excitation energy, the $B(E2;0^+_1\to 2^+_1)$ rate in $^{36}$Ca is larger. We found that in the threshold $2^+$ state, $^{36}$Ca is spatially difused, which accounts for the abnormal $B(E2)$ trend observed[2].[1] Z. C. Xu, S. Zhang, J. G. Li, et al. Phys. Rev. C 108, L031301 (2023)
[2] Z. C. Xu, S. M. Wang, T. Beck, et al. Phys. Rev. C 112, L011302 (2025)Speaker: Dr Zhicheng Xu (Fudan University) -
42
Emergence of High-Purity Spin-Triplet States and Quantum Entanglement in Proton–Proton Scattering
Entanglement is a unique feature of quantum mechanics that remains relatively unexplored in the context of nuclear physics. In this work, we investigate spin entanglement in elastic proton-proton scattering with unpolarized beams. By analyzing the final spin density matrix from the scattering amplitude, we find two regimes where the outgoing spin state has near-maximal purity: a known low-energy $S$-wave singlet-dominated region, and a new intermediate-energy region at $E_{\text{lab}}\approx151\,\text{MeV}$ and $\theta_{\text{c.m.}}\approx90^{\circ}$, with a highly pure spin-triplet configuration. We show that the triplet-dominated final state exhibits strong nonclassical correlations, violating the Bell inequality with substantial potential. Furthermore, we quantify the entanglement using concurrence and entanglement power, both of which peak in the same kinematic domain. These results demonstrate that unpolarized $pp$ scattering can serve as a practical source of entangled triplet spin states, offering a new platform for experimental tests of quantum nonlocality and to investigate the spin structure of the nuclear force.
Speaker: zhaoxin shen (Fudan University) -
43
Construction of 1S0 pair collective Hamiltonian using the constrained BCS + local QRPA method
One of the important correlations in atomic nuclei is pairing, where two nucleons form a pair. The pairing correlation can lead to a phase transition into a superfluid state, analogous to the superconducting state observed in electronic systems. In the superfluid phase, the global U(1) gauge symmetry is spontaneously broken. As a result, a new type of the collective mode emerges: the pair rotational mode (Nambu-Goldstone mode) which corresponds to the motion along the bottom of a wine-bottle-shaped effective potential, in addition to the pair vibrational mode which involves fluctuations in the magnitude of the order parameter.
In finite systems such as nuclei, phase transitions do not occur sharply due to significant quantum fluctuations. Instead, a critical state exists between the normal and the superfluid phase. Nuclei near closed-shell configurations are typically considered to exhibit pair vibrational modes. However, previous studies (Clark et al. 2006) have shown that some magic-number nuclei may actually be in a critical state.
To describe shape coexistence phenomena (Kris and John 2011) with quantum fluctuations, such as those observed in 98Kr, five-dimensional quadrupole collective Hamiltonian has been extensively used (Próchniak and Rohoziński 2009). In a similar spirit, describing nuclei in a pairing critical state requires the construction of a pair collective Hamiltonian that can simultaneously include both pair rotational and vibrational dynamics and their couplings. Despite its importance, research on pair collective Hamiltonians remains limited, with most models relying on simple monopole pairing interactions (Bes et al. 1970). Consequently, current approaches are restricted to narrow model spaces and can only be applied to a limited number of nuclei.To extend the applicability of the pair collective models to a wider range of nuclides, we aim to construct the pair collective Hamiltonian based on nuclear density functional theory. The potential energy surface is expressed as a function of the pairing gap (the collective variable), while the inertial functions, namely the pair rotational moment of inertia and the pair vibrational mass, are obtained using local QRPA calculations that account for the pairing gap dependence. We then construct a pair collective Hamiltonian that can describe the pair dynamics in the critical regime and allows us to reassess the stability of the magic nuclei from the perspective of the pairing correlations.
As a first step toward this goal, we have obtained the potential energy surface using BCS calculations with constraints on the pairing gap, employing monopole pairing interactions. In this presentation, we will also discuss the pairing gap dependence of the pair rotational moment of inertia and the pair vibrational mass using the local QRPA method.Speaker: Chisato Ruike (Pure and Applied Sciences, University of Tsukuba) -
44
Hypernuclear Structure and Hyperon Star Properties with Relativistic Density Functional Theory
Hypernuclear systems and neutron stars offer complementary environments for exploring baryon interactions across a wide range of densities. This report investigates $\Xi^{-}$ hypernuclear structure and the equation of state (EOS) of hyperon-rich matter using relativistic density functional theory. The structure of selected light $\Xi^{-}$ hypernuclei, such as $^{15}_{\Xi^{-}}$C and $^{13}_{\Xi^{-}}$B, are described within the density-dependent relativistic mean-field (DDRMF) framework, where the in-medium behavior of meson-hyperon couplings and the role of the isovector scalar $\delta$ meson are analyzed in detail. To extend the constraints toward supranuclear densities, experimental information from hypernuclei is incorporated into a Bayesian inference scheme. A statistically significant linear correlation between scalar and vector $\Xi N$ coupling strengths is established and used as a nuclear-physics prior. When combined with multimessenger astrophysical observations, including neutron star masses, radii, and tidal deformabilities, the resulting posterior distribution enables a more constrained and realistic description of hyperonic matter. This approach improves the stiffness of the EOS and supports the existence of $2M_{\odot}$ hyperon stars, offering new insights into the hyperon puzzle from a joint nuclear and astrophysical perspective.
Speaker: ShiYuan Ding (Lanzhou University) -
45
Quantum entanglement entropy: unveiling the shell evolution
We investigate the evolution of nuclear shell structure in neutron-rich isotopes through the lens of quantum information theory, using quantum entanglement entropy as a diagnostic tool. Employing shell model calculations, we compute both single-orbital and total correlation entropy for oxygen and calcium isotopic chains. Our results identify the emergence of new magic numbers at ( N=14, 16 ) in oxygen and ( N=32, 34 ) in calcium, evidenced by pronounced minima in total entropy. The single-orbital entropy further reveals orbital-level decoupling at these closures, confirming enhanced nuclear stability. Extending the analysis to iron, chromium, and nickel isotopes, we explore entanglement patterns near the merging regions of the islands of inversion around ( N=40 ) and ( N=50 ), highlighting collective effects. This study demonstrates that quantum entanglement measures provide a powerful, complementary perspective to conventional observables in tracing shell evolution and uncovering underlying correlations in exotic nuclei.
Speaker: Di Xu (School of Physics,Xi'an jiaotong university) -
46
(Cancelled) Toward global calculations for charge-exchanging processes using Gogny energy density functional
Charge-exchanging processes such as beta decay, neutrinoless double-beta decay, and Gamow-Teller giant resonances are observed in a wide region of the nuclear chart and play important roles in nuclear physics and related fields. Theoretical descriptions based on nuclear density functional theory (DFT) enable us to calculate all the nuclei in the chart. A standard approach for describing charge-exchanging processes within nuclear DFT is the proton-neutron quasiparticle random-phase approximation (pnQRPA). QRPA is computationally demanding, as it involves the diagonalization of a large-dimensional matrix in its original formulation, but an efficient solution called the finite amplitude method (FAM) was developed recently [1]. The proton-neutron FAM (pnFAM) [2] has been successfully applied to beta decay, Gamow-Teller resonances, and two-neutrino emitting double-beta decay using Skyrme-type energy density functionals [3, 4].
In this presentation, we will present the current status of implementing the Gogny-type energy density functional, which has less uncertainty in the proton-neutron pairing channel than the Skyrme-type one, into the pnFAM code to calculate the transition strength for charge-exchanging processes.[1] T. Nakatsukasa, T. Inakura, and K. Yabana, Phys. Rev. C 76, 024318 (2007).
[2] M. Mustonen, T. Shafer, Z. Zenginerler, and J. Engel, Phys. Rev. C 90, 024308 (2014).
[3] M. Mustonen and J. Engel, Phys. Rev. C 93, 014304 (2016).
[4] N. Hinohara and J. Engel, Phys. Rev. C 105, 044314 (2022).Speaker: Kenta Akai (University of Tsukuba)
-
37
-
33
-
-
47
Ab initio methods for nuclear structure (4/4)
-
10:50
break
-
48
Quantum many-body formulation of nuclear shapes, rotations, and vibrations (3/4)
-
11:55
break
-
49
in-beam gamma-ray spectroscopy in the era of GRETA (tentative) (3/4)
-
14:20
break
-
50
Probing buclear structure with electron beam (TBC)
-
15:25
break
-
Young Scientist Session 4
-
51
Advanced Signal Processing for Transient Oscillations
Experimental physics often involves detecting weak, time-varying signals embedded in noise-challenges common to both nuclear and biomedical systems. This work explores techniques for extracting and analyzing non-sinusoidal oscillations in noisy, multichannel datasets. Using time-frequency analysis and adaptive denoising methods, we address issues such as amplitude and frequency modulation, phase deviation, and transiet signal detection.
Originally applied to physiological data mimicking dynamic pressure changes in biological systems, these tools are broadly applicable to nuclear epxeriments, including beam diagnostics, gamma-ray detection, and rare eent analysis. The methods enhance signal fidelity and temporal resoltion, offering framework that could improve the acccuracy and interpreability of experimental data in complex, noisy environments.
Speaker: Mr abdikarim abdi (Washington University) -
52
Research on high time resolution pulsed slow positron beam technology and its applications
Pulsed slow-positron beams enable atomic-scale characterisation of surface and near-surface microdefects, furnishing precise data on defect size, concentration and spatial distribution. This study establishes a high brightness, high time resolution pulsed slow positron platform based on a solid-neon moderator that incorporates two distinct pulsing technologies within a common magnetic transport line. The first approach employs an integrated three-stage pulsing unit—comprising a chopper, prebuncher, and buncher—to generate a pulsed slow-positron beam with a count rate of 13 000 cps and a time resolution of 187 ps. The second approach combines a Penning-trap accumulation scheme with a buncher to generate positron burst with 600 ps time resolution, and a dedicated 2048-channel array detector has been developed to accommodate the resulting high-intensity gamma bursts. Together, the two pulsed slow-positron beamlines established in this study provide a versatile, high-resolution probe for nanoscale surface and near-surface physics, while high-brightness positron bursts also hold definite significance for advancing antimatter research.
Speaker: Xiaotian Yu (Institute of High Energy Physics, Chinese Academy of Sciences) -
53
Performance Evaluation of the Ion Chambers for a Wide Range of Atomic Numbers in the RIKEN TRIP-S3CAN Experiment
In the RIKEN TRIP-S3CAN experiment, a series of measurements has been initiated to determine interaction and charge-changing cross sections over a wide range of atomic numbers (Z). The particle identification capability for heavy ions plays an important role in this experiment. By applying velocity corrections to the energy loss measured with ionization chambers, the atomic number of each particle can be determined. In this study, newly developed ionization chambers at F3 and F8 were installed, in addition to the standard ionization chambers located at focal planes F7 and F11. In this presentation, we discuss the performance evaluation of these ionization chambers in the Z = 25–60 region.
Speaker: ka you (Tokyo city university) -
54
Developments of Radioactive Isotope Beams using Long-Lived Nuclides from Accelerator Mass Spectrometry System
Accelerator Mass Spectrometry (AMS) can detect extremely small amounts of long-lived nuclides ($^{10}$Be, $^{14}$C, $^{36}$Cl, $^{129}$I, etc.) in sample. It is applied for studies of environmental dynamics using seawater or rainwater, cosmic ray event exploration using Antarctic ice core and so on.
We have been developing RI beams using long-lived nuclides provided from the AMS system at the University of Tsukuba Tandem Accelerator Complex (UTTAC) for experiments of nuclear physics.
We developed $^{10}$Be and $^{14}$C beams. In the AMS, an ionization chamber (IC) is used to count the number of rare isotopes, and an absorber gas is used to remove isobaric interferences. Considering the use of the beam for nuclear physics, it is desirable to minimize the energy loss and maintain the beam energy as much as possible. Therefore, we investigated the response of the gas detector when the gas pressure of the P10 gas in the IC, and the argon gas in the absorber cell were reduced. We also examined the beam size. The count rate is also important for beam utilization, and we are trying to improve the isotope ratio of $^{10}$Be by preparing samples with rainwater.Speaker: Misaki Mikawa (University of Tsukuba) -
55
Development and Full Realization of PLASEN: Precision Laser Spectroscopy for Exotic Nuclei
Z. Yan1, X. F. Yang1, on behalf of PLASEN collaboration
1School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China.
The study of exotic structures in unstable nuclei lies at the forefront of nuclear physics [1]. The fundamental properties of these nuclei are intimately related to nuclear structure and nucleon-nucleon interactions, making them crucial for exploring a variety of exotic phenomena, including halo structure, island of inversion, and shell evolution. Laser spectroscopy can accurately measure the hyperfine structure and isotope shifts of atoms and ions, enabling the extraction of fundamental nuclear properties such as spins, magnetic moments, electric quadrupole moments, and charge radii in a nuclear-model-independent manner [2]. Among various laser spectroscopy techniques, collinear resonance ionization spectroscopy is distinguished by its high resolution and sensitivity, offering a powerful approach for studying unstable nuclei and evaluating nuclear structure models.
Our group focuses on developing advanced laser spectroscopy systems for radioactive ion beam facilities in China [3-4]. Currently, we have successfully established PLASEN (Precision Laser Spectroscopy for Exotic Nuclei), a fully functional high-resolution and high-sensitivity collinear resonance ionization laser spectroscopy system for off-line and on-line experiments. In off-line experiments, multiple lasers were employed for the excitation and ionization of the corresponding atoms, and optimal schemes with the highest efficiency were chosen. Under these conditions, the hyperfine structure spectra of 85, 87Rb and 133Cs were successfully measured [5-6]. With these experimental configurations established, on-line experiments have recently been conducted at BRIF in China, where the hyperfine structure spectra of unstable Rb isotopes have been measured.
In this presentation, the principles of collinear resonance ionization laser spectroscopy will be introduced, followed by an overview of the PLASEN setup. Recent on-line and off-line experimental configurations and results will be presented, along with an outline of future developments.
[1] Ye, Y., Yang, X., Sakurai, H. et al. Physics of exotic nuclei. Nat Rev Phys 7, 21–37 (2025). https://doi.org/10.1038/s42254-024-00782-5
[2] Yang, X., Wang, S., Wilkins, S. G. et al. Laser spectroscopy for the study of exotic nuclei. Prog Part Nucl Phys 129 (2023): 104005.
[3] Bai, S., Yang, X. et al. Commissioning of a high-resolution collinear laser spectroscopy apparatus with a laser ablation ion source. Nucl Sci Tech 33.1 (2022): 9.
[4] Wang, S., Yang, X. et al. Construction and commissioning of the collinear laser spectroscopy system at BRIF. Nucl Instrum Meth A 1032 (2022): 166622.
[5] Hu, H., Guo, Y. et al. Development and characterization of a high-resolution, high-sensitivity collinear resonance ionization spectroscopy system. Sci Bull (2025). https://doi.org/10.1016/j.scib.2025.06.036
[6] Guo, Y., Yan, Z. et al. Development of Cesium Laser Resonance Ionization Schemes for the PLASEN Experiment. Chin Phys C (2025). https://doi.org/10.1088/1674-1137/adf49eSpeaker: Zhou Yan (Peking University) -
56
Accelerating Nuclear Structure Studies: A ResNet-18 Machine Learning Approach for Event Classification in the MATE-TPC
The study of nuclear structure, particularly clustering phenomena in light nuclei such as Carbon-12 (¹²C), is essential for advancing our understanding of nuclear forces and stellar nucleosynthesis. Elastic and inelastic scattering reactions, like ¹²C(p,p)¹²C and ¹²C(α,α)¹²C, are powerful probes for investigating these fundatmental properties. The Active Target Time Projection Chamber (AT-TPC), such as the MATE-TPC developed at Institute of Modern Physics, offers comprehensive 3D tracking of reaction products, allowing for precise reconstruction of reaction kinematics and missing-mass spectra. However, the large volume and complexity of the resulting point-cloud data pose significant challenges for conventional data analysis methods, which are often labor-intensive and time-consuming.
To overcome this challenges, we have developed an automated event classification framework utilizing a deep convolutional neural network (CNN). In this work, we apply the ResNet-18 architecture to classify reaction events from ¹²C+p and ¹²C+α scatterings simulated with the MATESIM toolkit in the MATEROOT code. The 3D particle tracks “detected” by the MATE-TPC are projected onto 2D planes, generating image-like input for the network. Our trained model achieves high performance, attaining over 94% classification accuracy in distinguishing proton events from none-proton events. Analysis of the model's performance, including its confusion matrix, and examination of misclassified events demonstrate its robustness and identifies areas for further improvement. This deep learning approach greatly enhances the efficiency and objectivity of data analysis in AT-TPC experiments, paving the way for rapid processing of large datasets and enabling searches for rare reaction channels that are essential for advancing nuclear physics research.
Speaker: ZhiHeng Hu (Institute of Modern Physics,Chinese Academy of Sciences) -
57
Status of R&D activities for FAZIA detector upgrade in Korea
FAZIA (Forward-angle A and Z Identification Array) is a multi-detector array designed to identify charges and masses of the reaction fragments from heavy ion collisions in the Fermi energy domain. One basic unit of FAZIA detector consists of three layers which include two Si sensors with different thicknesses and one CsI scintillator detector read out by a photodiode, forming the FAZIA telescope. The detector signals are analyzed using digital signal processing implemented on FPGAs, which are integrated into the front-end electronics board (FEB). The telescope structure enabled the charge identification of nuclei with Z up to 54 and the isotopic nuclei discrimination with Z up to 25 by using the ∆E - E information and Z up to 20 with the pulse shape analysis. A single FAZIA detector module consists of 16 telescopes.
The FAZIA upgrade project began a few years ago with the goal of extending beam-energy coverage and enhancing acceptance. The Korean FAZIA team takes major responsibility for developing new Si sensors with various thicknesses and improving the performance of FEBs. The Si sensors, designed through TCAD simulations, have been successfully fabricated and tested for their I-V characteristics and performance using an Am-241 source. Additionally, prototype FEBs have been developed using modern FPGA chips and other advanced components. New VHDL code has also been developed. The testing system for prototype detectors and FEBs is complete at present. This presentation will highlight recent efforts by the team in the upgrade project, with a particular focus on the R&D of new Si sensors and electronics.Speaker: Giyeong Kim (Inha University (KR)) -
58
Development of an active target TPC for studying alpha cluster structure in 12C and 16O
We aim to investigate alpha-clusters in alpha-conjugate nuclei, such as 12C and 16O, using the Active-Target Time Projection Chamber (AT-TPC). Performance test of prototype AT-TPCs were conducted using a 200 MeV/u carbon beam at the Heavy Ion Medical Accelerator in Chiba (HIMAC). The results from this test provide valuable insights for the development and optimization of the Sejong TPC-Drum, which will be utilized in the Large Acceptance Multi-Purpose Spectrometer (LAMPS) experiment for low-energy studies at RAON. In this presentation, we report on the performance results of the prototype AT-TPCs and the current status of the Sejong TPC-Drum.
Speaker: Seonggeun Hwang (Sejong University)
-
51
-
Young Scietist Session 5 (Poster)
-
59
Quarkyonic matter with chiral symmetry restoration
We present a novel unified approach to describe the dense symmetric nuclear matter by combining the quarkyonic matter framework with the parity doublet model. This integration allows for a consistent treatment of the transition from hadronic to quark degrees of freedom while incorporating chiral symmetry restoration effects. Our model introduces a chiral invariant mass for both baryons and constituent quarks, enabling a smooth crossover between hadronic and quark matter in symmetric nuclear matter. We derive the equation of state
(EOS) for this hybrid system and investigate its thermodynamic properties. The model predicts a gradual onset of quark degrees of freedom at high densities while maintaining aspects of confinement.Speaker: Bikai Gao (RCNP, Osaka University) -
60
Antisymmetrized molecular dynamics for exotic nuclear structures
Antisymmetrized Molecular Dynamics (AMD) has emerged as a powerful microscopic framework for investigating exotic structures in unstable nuclei, especially those near the drip lines. Unlike traditional mean-field models, AMD treats each nucleon as a Gaussian wave packet, allowing the emergence of deformation, clustering, and halo phenomena from first principles without assuming predefined symmetries. This work presents a comprehensive study of exotic nuclear structures—including α clustering, neutron and proton halos, skin effects, and shape coexistence—within the AMD framework. We want to explore the structural evolution in light to medium-mass nuclei, analyze the impact of weak binding and continuum coupling, and highlight the role of isospin asymmetry and shell evolution. Our results will compared with experimental observables such as radii, energy spectra, and transition strengths, demonstrating the versatility of AMD in capturing the complex dynamics of exotic nuclei. This study underscores the importance of microscopic approaches in advancing our understanding of nuclear structure at the limits of stability.
Speaker: Prof. Siming Wang -
61
Neutron Irradiation Effects on SiPM
Silicon Photomultipliers (SiPMs), which operate in Geiger mode, are widely used in high energy physics experiments due to their excellent photon detection capabilities. However, their performance can degrade when exposed to high radiation environments which may significantly impact experimental results.
In this study, we investigate the radiation induced performance degradation of two different types of SiPMs by comparing their characteristics before and after neutron irradiation. Key performance metrics including IV characteristics, single photon electron, and LED Response current levels were measured and analyzed. The results provide insights into the radiation hardness of each SiPM model and offer guidance for their application in radiation rich environments.Speaker: Mr JunHyung Park (Department of Physics, Kyungpook National University) -
62
Development of an MR-ToF combined with Inductively Coupled Plasma Mass Spectrometry at the University of Manchester
The laser spectroscopy group at the University of Manchester aims to realise a combination of Inductively Coupled Plasma Mass Spectrometry (ICP-MS) with a Multi-Reflection Time-of-Flight Mass-Spectrometer (MR-ToF).
The MR-ToF has in recent decades become a powerful technique for high-precision mass measurement of exotic nuclides at RIB facilities, using multiple reflections of an ion cluster to extend the flight path up to 1000s of times, demonstrating mass resolution of over $m/Δm = 10^{6}$. In combination with an ICP-MS source, the superior mass resolving power and dynamic range of the MR-ToF can be applied to ultra-trace analysis of low-level waste. The proposed spectrometer will include a region of laser overlap for selective ionisation of the ICP-MS output, enhancing the chemical selectivity of the instrument.
I will present the current status of this spectrometer under construction at UoM, and the development of a linear cooler-buncher, which will create pulsed ion bunches nanoseconds in width for injection into the laser spectroscopy and MR-ToF stages.Speaker: Emily Agg (University of Manchester) -
63
Current Status of The Segmented La-GPS Scintillation Crystal Detector as a New Implant-β Detection Tool at Fragmentation Facilities
The rapid neutron capture (r-) process holds a significant amount of interest as a means for nucleosynthesis of elements in astrophysical environments. From the perspectives of both nuclear physics and astrophysics, ongoing efforts are being carried out to better understand it. Such efforts include the measurements of β-decay and delayed neutron emissions of the r-process elements in order to obtain a more accurate input for the calculations in relation to its theoretical modelling [1].
Typically, β-γ spectroscopies are conducted with implantation detectors at fragmentation facilities such as the implementation of the Silicon Strip Detectors (SSDs) at Radioactive Isotope Beam Factory (RIBF). However, SSDs are incapable of fast timing response for the purpose of neutron time-of-flight measurements of the delayed neutron emissions. Therefore, to address this limitation, the Yttrium Orthosilicate (YSO) segmented scintillation crystal detector (Z ≈ 35, ρ ≈ 4.5 g/cm3) was developed. The characteristics of the YSO allow for 80% correlation efficiency with 3mm correlation radius between implant events and β-decay events [2].
The success of the YSO prompted the development of the Lanthanum-enriched Gadolinium Pyrosilicate (La-GPS) segmented scintillation crystal detector (Z ≈ 51, ρ ≈ 5.2 g/cm3) to achieve better correlation radius and higher energy resolution compared to the YSO, and faster timing response than SSDs [3]. This presentation will then showcase the current status of the La-GPS scintillation crystal detector of (1.5 x 1.5)mm arranged into a 32 x 32 array in the x-y plane.References
- M. R. Mumpower et al., “The impact of individual nuclear properties on r-process nucleosynthesis,” Prog. in Particle and Nucl. Phys., vol. 86, pp. 86-126, 2016.
- R. Yokoyama et al., “Segmented YSO Scintillation Detectors as a New β-Implant Detection Tool for Decay Spectroscopy in Fragmentation Facilities,” Nucl. Instrum. Methods Phys. Res. A, Accel. Spectrom. Detect. Assoc. Equip., vol. 937, pp. 93–97, 2019.
- A. Suzuki et al., “Fast and high-energy-resolution oxide scintillator: Ce-Doped (La,Gd)2Si2O7,” Appl. Phys. Express, vol. 5, no. 10, p. 102601, 2012.
Speaker: Yasmin Anuar -
64
A new Hamiltonian for jj4_45 model space and corresponding spectroscopic study
This study advances the nuclear shell model by systematically investigating effective interactions in the f5pgd5 shell region (mass numbers 40 < A < 100).
Building on existing interactions(JUN45 and jj45pna), we refine central, spin-orbit, and tensor force parameters, incorporating universal monopole corrections to develop the first dedicated effective interaction for the f5pgd5 region. Validation near the N=50 shell closure demonstrates excellent agreement with experimental data and superior performance over existing models, confirming its applicability across this region and beyond.
Leveraging the optimized interaction, we generate a high-precision theoretical database for nuclides in this mass range, encompassing binding energies, excitation spectra, level densities, β-decay properties, and spectroscopic factors. Our work provides a foundational tool for future studies in nuclear structure and reaction physics, bridging theory and experiment in medium-mass nuclei.Speaker: 润泽 张 (中山大学) -
65
Combining Improved Thermoluminescence (TL) Dating and Nuclear Techniques for The Study of Ancient Sites
The report presents an overview on the combination of improved thermoluminescence (TL) dating and nuclear techniques - such as neutron activation analysis (NAA) and isotope ratio analysis - for the study of ancient sites. Applications of these techniques for ancient architectures built by bricks, stones and their challenging issues. Our recent improved thermoluminescence (imTL) technique is introduced in this study as an optimal solution for dating of ancient architectures having heterogeneous, multilayered and overlapped structures with highly reliable results compared to traditional TL methods. Besides, neutron activation analysis (NAA) and isotope ratio analysis are helpful for our study of ancient sites. We also briefly introduce in this study the important role of The Oc Eo-Ba The relic, the White Stone Citadel archaeological site and the Nguom rock shelter in the historical and archaeological aspects, based on which our improved TL dating technique can be applied.
Speaker: Ms Nguyen Thi Ngoc Hue (Center for Nuclear Technology Hochiminh City) -
66
Development of <sup>12</sup>C-enriched irradiation-resistant diamond targets for astrophysical <sup>12</sup>C(α, γ)<sup>16</sup>O reaction measurements
The 12C(α, γ)16O reaction plays a pivotal role in nuclear astrophysics research. The direct measurement of this reaction remains particularly challenging due to its extremely low cross section (approximately 10-17 barn at 300 keV) within the Gamow window. This study addresses the critical need for irradiation-resistant 12C-enriched targets to enable accurate measurements. We successfully fabricated a 12C-enriched diamond target on molybdenum substrate through Microwave Plasma Chemical Vapor Deposition (MPCVD), demonstrating remarkable stability under high-intensity proton beam irradiation. Experimental results revealed only a 1.8% decrease in the 12C(p, γ)13N reaction yield in the 12C layer following proton bombardment at 270 keV with 2 mA beam current and a total accumulated charge of 124.2 C, indicating a significant improvement compared to conventional carbon targets. Isotopic analysis confirmed a 13C/12C ratio of (9.7 ± 1.3) × 10-5, verifying the absence of contamination during MPCVD processing. Additionally, we developed a novel nuclear-reactionbased methodology for quantifying hydrogen content in thin films, establishing an upper limit of 0.058% (95% confidence level) for hydrogen concentration in the diamond target. The combined irradiation resistance and isotopic purity of this target meet the stringent requirements for direct 12C(α, γ)16O reaction measurements in astrophysical environments.
Speaker: Jing-Yu Dong (China Institute of Atomic Energy) -
67
Proton Emission Phenomenon of the Deformed Nuclide 185Bi
As a proton-emitter located beyond the proton drip line, $^{185}\mathbf{Bi}$ possesses unique properties, such as susceptibility to deformation, continuum effects, etc. A recent experiment confirmed the $1/2^+$ ground state, but left long-lived isomeric state hard to explain. The study of proton emission can promote a large number of exotic phenomena and new physics. The difficulties in experimental measurement brought about by low reaction cross-sections and short half-lives provide opportunities and challenges for related theoretical studies. Its achievements will also lay the foundation for future research and provide certain guiding.
The GCC method is used, while a deformed proton-emitter is constructed using the particle-rotor model, and it is expanded in complex momentum space using Berggren basis. As Berggren basis includes bound and unbound states, the wave functions of the internal and asymptotic regions can be processed in a unified framework, thereby introducing the continuum effect.
Taking $^{185}\mathbf{Bi}$ as the research object, we calculate the variation of the single particle energy level of the core with deformation. By comparing it with the Nilsson energy level, the Thomas-Ehrman effect is studied. Further, the energy spectrum of $^{185}\mathbf{Bi}$ under different deformation parameters is calculated. The calculated energy spectrum is cross checked with the results obtained by the TRS method, reproducing the $1/2^+$ ground state measured in the experiment, and the ground state should be formed by a long ellipsoidal nucleus of $β_2≈0.3$. In a nearly spherical case, it is highly likely that there are two $7/2^-$ state and $9/2^-$ state.Speaker: Qingyuan Xu -
68
Polarised Deuteron Breakup as a Probe of the Nuclear Symmetry Energy
The Nuclear Equation of State (EoS) provides a fundamental link between nuclear physics and astrophysics, yet its predictive power is limited by our incomplete understanding of the nuclear symmetry energy, $E_\text{sym}(\rho)$. This critical component, which quantifies the energy cost of proton–neutron asymmetry, is well constrained at the saturation density found in stable nuclei, but remains a major uncertainty at the sub-saturation and supra-saturation densities relevant to neutron stars. This uncertainty leads to significant discrepancies in astrophysical models, particularly those predicting the mass–radius relationship of neutron stars.
This research outlines a novel laboratory experiment designed to directly constrain the symmetry energy, reducing our reliance on rare astrophysical observations. The core of the approach is to use the Improved Quantum Molecular Dynamics (ImQMD) framework to model the peripheral collision of a polarised deuteron with a heavy, neutron-rich target. The isovector force - a component of the strong nuclear interaction that distinguishes between protons and neutrons - acts attractively on the deuteron’s proton and repulsively on its neutron. These opposing forces cause the two nucleons to scatter at different angles.
The resulting difference in scattering angle serves as a highly sensitive probe of the symmetry energy’s "stiffness", a property parameterised by the variable $\gamma$ in the model. By measuring the differential cross-sections of the outgoing protons and neutrons in an experiment conducted at RIKEN’s Radioactive Isotope Beam Factory (RIBF) using the SAMURAI spectrometer, the data can be compared to a library of ImQMD simulations. This comparison enables the determination of the $\gamma$ value that best fits the experimental results, providing a new and precise constraint on the nuclear symmetry energy — and ultimately refining our understanding of nuclear matter, from the laboratory to the cosmos.
Speaker: Zichen Luo (Department of Physics, Tsinghua University) -
69
Multi-photon Propagation in an X-ray Cavity with Resonant Nuclei
With the development of the X-ray source, stimulating nuclear quantum states directly becomes possible experimentally with synchrotrons and XFELs. The collective behaviors of the stimulated nuclear ensemble were studied theoretically in the past decade as a new frontier of nuclear science and quantum science. With specific numerical method and theoretical model, the correlation between scattering photons by the nuclear ensemble are the topic of my interest.
Speaker: Boyi Deng (University of Chinese Academy of Science) -
70
Momentum kick model with multiplicity dependence in pp collisions and p-Pb collisions
The long-range near-side ridge phenomenon in two-particle correlation(∆φ-Δη) is one of powerful tools in exploring strong interaction. Although the hydrodynamic model describes this ridge structure in heavy ion collisions, this could not offer the explanation that ridge phenomenon occurs in the small systems such as pp collisions and p-Pb collisions because density and temperature are not enough to generate a hydrodynamic medium. The Momentum Kick Model (MKM) explains this effect via high-momentum jet particles transferring momentum to medium partons, inducing collective motion. We extend MKM to momentum kick model with multiplicity dependence (MKMwM), which is the MKM considering the average number of kicked partons with an impact parameter, using new experimental data to analyze and predict ridge structures in pp collisions and p-Pb collisions at the LHC.
Speaker: Hyeongwoo Noh (Inha University) -
71
Accurate velocity determination of stored ions in CSRe by correcting the non-isochronicity of time-of-flight detectors
Accurate velocity determination of stored ions in storage rings plays a key role for nuclear mass measurements using the technique of B$\rho$-defined isochronous mass spectrometry (B$\rho$-IMS). However, the accuracy and precision of the ion's velocity are seriously deteriorated by the non-isochonicity of the time-of-flight (TOF) detectors. In this paper, the non-isochonicity is described by a correlation function between the time-delay difference, $t_d$, of the two TOF detectors and the orbital length, $C$, of the stored ions. The obtained correlation functions, $t_d\sim C$, allow for accurate determination of the ion's velocity which is then used for mass calibration in the B$\rho$-IMS technique. The present data analysis method is proved to be capable of resolving the effects of the non-isochronicity of TOF detectors.
Speaker: Jinyang Shi -
72
Resonance of K*0(892) in and out of jets in pp collisions at sqrt(s) = 13.6 TeV
Recent measurements of two-particle correlations within jets in high-multiplicity pp collisions at √s = 13.6 TeV reveal flow-like patterns among jet constituents. Such effects were previously considered unique to heavy-ion collisions, suggesting that a hot, dense QCD medium may form even inside jets in small systems. As this medium hadronizes, substantial final-state hadronic interactions can persist, leading to significant modifications of short-lived resonance yields through (pseudo-)elastic scatterings with other hadrons after chemical freeze-out. To investigate this, we analyze yields of the short-lived K⁰ meson using high-multiplicity jets in pp collision data at √s = 13.6 TeV collected by the ALICE Collaboration during LHC Run 3. Charged-particle jets are reconstructed, and per-jet K⁰ yields are measured in and out of the jet cone. Comparing these yields for this resonance offers new insight into final-state hadronic interactions inside jets produced in small collision systems.
Speaker: Jimun Lee (Sejong University) -
73
Status of the Si-detector development for FAZIA
A unit detector of the FAZIA(Forward-angle A and Z Identification Array) telescope consists of three layers with two silicon sensors and a CsI scintillator. The silicon sensors measure the energy loss of charged particles passing through or stopped in the detector. The FAZIA detector can distinguish charges up to Z = 52 and isotopes up to Z = 25 by using ΔE-E correlation and the pulse shape analysis (PSA). The Korean FAZIA group has developed silicon sensors with the thickness of about 750 and 115 μm, employing various configurations. The energy resolutions measured by using the Am-241 alpha radiation source can provide one of the criteria for adoption. In this presentation, the characteristics of the prototype FAZIA silicon chips, measured by using the Am-241 source, are presented.
Speaker: Mr Wonjun Jeong (INHA university) -
74
Calibration and Simulation of the Proton Polarimeter 2nd-FPP and Track Calibration using Cosmic Rays
Nucleon–nucleon (NN) interactions inside nuclei are expected to be modified by nuclear medium effects. To investigate these effects, we are developing the focal-plane proton polarimeter (2nd-FPP), designed to measure proton polarization via the left–right asymmetry in elastic p–¹²C scattering, with particle tracking provided by multi-wire drift chambers (MWDCs).
A calibration experiment at RCNP successfully separated p–¹²C events from p–p events; however the effective analyzing power in the forward angular range was lower than reference values. GEANT4 simulations incorporating polarization effects reproduced this result, indicating that the discrepancy is likely due to overestimated scattering angles caused by bulging of the MWDC window films. To address this issue, we are calibrating the drift-time–to-distance relationship using cosmic rays. TThe progress of this calibration will be reported.Speaker: 佐藤 多恵 (九州大学大学院理学府物理学専攻)
-
59
-
47
-
-
75
in-beam gamma-ray spectroscopy in the era of GRETA (tentative) (4/4)
-
10:50
break
-
76
Quantum many-body formulation of nuclear shapes, rotations, and vibrations (4/4)
-
Closing Ceremony
-
75