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Journal Articles

Double-differential cross sections for charged particle emissions from $$alpha$$ particle impinging on Al at 230 MeV/u

Furuta, Toshimasa*; Uozumi, Yusuke*; Yamaguchi, Yuji; Iwamoto, Yosuke; Koba, Yusuke*; Velicheva, E.*; Kalinnikov, V.*; Tsamalaidze, Z.*; Evtoukhovitch, P.*

Journal of Nuclear Science and Technology, 61(2), p.230 - 236, 2024/02

 Times Cited Count:0 Percentile:0.01(Nuclear Science & Technology)

Charged particle production from $$alpha$$ particle fragmentation reactions was investigated experimentally by measurement of 230-MeV/u $$alpha$$ particles bombarding an aluminum target. Double differential cross sections were measured for each ejectile of p, d, t, $$^{3}$$He, and $$^{4}$$He at laboratory angles between 15 and 60 deg. The results of analyzed data found the following common characteristics: (1) spectra of proton- and neutron-emission are similar in high energy region at forward angle, (2) triton-to-$$^{3}$$He ratio of $$alpha$$-breakup yield is 1:2, which is similar to lower incident energy experiment, and (3) the shape of broad peak formed by $$^{3}$$He and $$alpha$$ particles could be explained by the process with collision between induced $$alpha$$ particle and target nucleus.

JAEA Reports

Proceedings of the 2021 Symposium on Nuclear Data; November 18-19, 2021, On-line Connection Conference

Yamaguchi, Yuji; Meigo, Shinichiro

JAEA-Conf 2022-001, 226 Pages, 2022/11

JAEA-Conf-2022-001.pdf:17.97MB

The 2021 Symposium on Nuclear Data was held as an online connection conference on November 18-19, 2021. The symposium was organized by the Nuclear Data Division of the Atomic Energy Society of Japan (AESJ) in cooperation with the Sigma Investigative Advisory Committee of AESJ, J-PARC Center, Nuclear Science and Engineering Center of Japan Atomic Energy Agency (JAEA), and High Energy Accelerator Research Organization (KEK). In the symposium, tutorials "New Developments in TALYS and TENDL-2021" and "Role of ADS and its Development Issues" were proposed and held. Three sessions of lectures and discussions were held: "J-PARC and JAEA Facilities", "Current Status and Future Prospects of Nuclear Data Research", and "Medical, Isotope Production, and Analysis". In addition, recent research progress on experiments, nuclear theory, evaluation, benchmark, and applications were presented in the poster session. The total number of participants was 132 participants. Each oral and poster presentation was followed by an active question and answer session. This report consists of a total of 36 papers including 14 oral and 22 poster presentations.

Journal Articles

Deuteron-induced nonelastic cross sections based on the intranuclear cascade model with independent incident particles under interaction potentials

Nakano, Masahiro*; Yamaguchi, Yuji; Uozumi, Yusuke*

Physical Review C, 106(1), p.014612_1 - 014612_8, 2022/07

 Times Cited Count:0 Percentile:0.02(Physics, Nuclear)

Deuteron-induced nonelastic cross sections are studied in an extended intranuclear cascade (INC) model. A three-body framework of proton, neutron, and target is introduced into the INC model to incorporate naturally the decomposition and capture reactions from weakly bound deuterons. This framework includes three types of interaction potential, namely proton-target, neutron-target, and proton-neutron, the last of which causes the two nucleons in the deuteron to oscillate and play an important role in its breakup. The calculated results reproduce well the experimental data for $$^{12}$$C, $$^{40}$$Ca, $$^{58}$$Ni, and $$^{208}$$Pb targets with almost the same parameters as those determined previously for nucleon-induced nonelastic reactions.

Oral presentation

$$alpha$$-particle breakup at incident energy of several hundreds of MeV/u

Yamaguchi, Yuji*; Araki, Yusuke*; Fujii, Motoharu*; Watanabe, Gaku*; Sanami, Toshiya*; Matsufuji, Naruhiro*; Koba, Yusuke*; Iwamoto, Yosuke; Uozumi, Yusuke*

no journal, , 

For heavy-ion cancer therapy with carbon, there is a problem about radiation exposure due to secondary particles produced by heavy ion incident reaction. We have a plan to extend our improved intra nuclear cascade (INC) model for proton incidences to INC model for alpha and carbon incidences. However, there is no experimental data about multi-particle (proton, deuteron, triton, $$^{3}$$He and alpha) production double differential cross sections (DDXs) for alpha incident reactions to validate the extended INC model. In this work, we measured multi-particle production DDXs for 100 and 230 MeV/nucleon alpha incident reactions on samples (C, Al, Co, Nb) at the HIMAC building in National Institute of Radiological Sciences (NIRS), QST. As a result, we found that results calculated by the extended INC model agreed with experimental data at 30 degrees and those underestimated the experimental data with increasing angles.

Oral presentation

Beam loss monitor using nuclear reaction with high threshold-energy in the vicinity of J-PARC muon target

Yamaguchi, Yuji; Meigo, Shinichiro; Oi, Motoki; Harada, Masahide; Haga, Katsuhiro

no journal, , 

At the MLF of J-PARC, 1-MW proton beam with 3 GeV is injected into graphite and mercury targets which are aligned in a cascade scheme. The 2-cm-thick graphite target for muon production is placed upstream of the mercury target and emits radiation from proton injection. Although shielding is performed, the beam loss monitor in the vicinity of the muon target detects the radiation as a background event. To detect beam loss accurately, we have started to develop a new counting tube with bismuth foil to distinguish between beam loss events and background events.

Oral presentation

Measurement of radioisotope production by muon capture

Yamaguchi, Yuji; Harada, Masahide; Kawamura, Naritoshi*; Haga, Katsuhiro

no journal, , 

A negative muon ($$mu$$$$^{-}$$) is captured by a nucleus in many cases when the $$mu$$$$^{-}$$ enters the material. After the nuclear capture, a highly excited (Z-1) nucleus is produced and de-excites via the emission of neutrons and $$gamma$$-rays. Because this process can make radioisotpes, the material can be activated. To handle the activated sample safely and properly in the MLF, it is important to estimate its radioactivity accurately. The estimation can be performed using Monte-Carlo simulation code, PHITS. Because the reliability of PHITS results has an impact on radiation safety, benchmark of calculation is required. However, the calculation results cannot be verified due to limited data in terms of Z. It is confirmed that there exist discrepancies between calculation and experimental data. Therefore, comprehensive data of radioisotope production are desired. In this presentation, we report on the preliminary experiment to establish methodology for taking comprehensive data.

Oral presentation

Oral presentation

Measurement of $$alpha$$ of 230 MeV/u incident charged particles production double differential cross section

Furuta, Toshimasa*; Uozumi, Yusuke*; Yamaguchi, Yuji; Iwamoto, Yosuke; Sanami, Toshiya*; Koba, Yusuke*

no journal, , 

no abstracts in English

Oral presentation

Development of proton spectrometer using Cherenkov photons, 1

Meigo, Shinichiro; Nakano, Keita*; Yamaguchi, Yuji; Otsuji, Kenichi*

no journal, , 

no abstracts in English

Oral presentation

Preliminary experiment for measurement of radioisotope production from negative muon capture

Yamaguchi, Yuji; Harada, Masahide; Kawamura, Naritoshi*; Haga, Katsuhiro

no journal, , 

no abstracts in English

Oral presentation

Fixed measurement of thermal neutron intensity with gold-foil activation method at the J-PARC spallation neutron source

Harada, Masahide; Oikawa, Kenichi; Tsuchikawa, Yusuke; Yamaguchi, Yuji; Haga, Katsuhiro

no journal, , 

In the spallation neutron source at Materials and Life Science Experimental Facility in J-PARC, a 3-GeV and 1-MW proton beam induces into a mercury target and the neutrons beam is provide to neutron instruments. The target vessels are regularly replaced due to pitting damage. The proton beam power is gradually increased to 800 kW as of June 2022, and the optimum proton beam profile is used depending on the beam power. Based on these observations, fixed-point measurements have been periodically carried out to observe the intensity of the neutrons supplied from the spallation neutron source under the same measurement conditions at NOBORU. In the fixed-point measurements, the activation method with gold foils (15x15x0.1mm$$^3$$) was used to observe the absolute intensity of thermal neutrons with and without cadmium foil. The irradiation time was set to about 10 to 30 minutes in accordance with the proton beam intensity. The gamma-ray from irradiated foil was measured with a germanium detector, and the amount of activation was identified. As a result of the measurement, the thermal neutron intensity was slightly dependent on the proton beam intensity.

Oral presentation

Measurement of delayed neutrons from J-PARC spallation neutron source

Harada, Masahide; Teshigawara, Makoto; Oi, Motoki; Yamaguchi, Yuji; Oikawa, Kenichi; Tsuchikawa, Yusuke; Haga, Katsuhiro

no journal, , 

At J-PARC 1MW spallation neutron source, pulsed neutrons included by 25Hz pulsed proton beam are provided to neutron instruments. Recently, 800 kW proton beam operation is successful, and the proton beam power gradually increases. A neutron instrument observed neutron beams with weak time correction to proton pulse. Therefore, at the neutron instrument to measure neutron pulse characteristics, NOBORU, we tried to measure delayed neutrons. In the measurement, a neutron detector was located on the beam axis in the NOBORU experimental room and pulsed neutrons were measured with flight time after the beam operation stop. Pulse height was also measured to distinguish whether neutron or others. From the results, neutrons could be measured after the beam operation stop. We will present in details in the conference.

Oral presentation

Remote handling test of Moderators and Reflector in J-PARC MLF

Oi, Motoki; Yamaguchi, Yuji; Teshigawara, Makoto; Naoe, Takashi; Kikuchi, Yoshinori*; Yasuhara, Toshiyuki*; Saruta, Koichi; Kinoshita, Hidetaka; Harada, Masahide

no journal, , 

In the neutron source of the Materials and Life Science Experimental Facility (MLF) in J-PARC, a reflector and three moderators are installed. Life time of the reflector and moderators are designed as 30,000 MWh. Spent moderators and reflectors are highly radioactive, so it must be replaced remotely. It has already been 15 years since the first beam of the MLF. Remote handling test was conducted in 2021 and 2022 using spare moderator and reflector in MLF's hot cell. In the remote handling test, there are some problems to replace irradiated moderators. It was found that there is a risk of damage to the poisoned moderator during installation and removal process. In addition, it was found that some slings were deformed and affected the work. Regarding the confirmed problems, we will make appropriate improvements and conduct a remote handling test again during the maintenance period in 2023. The replacement work of the actual moderators are scheduled to be carried out in 2024.

Oral presentation

Oral presentation

Irradiation test for material of proton beam window at MLF

Yamaguchi, Yuji; Meigo, Shinichiro; Okubo, Nariaki; Oi, Motoki

no journal, , 

no abstracts in English

Oral presentation

Measurement of intensity and spatial distribution of thermal neutrons with the large-area gold-foil activation method at the Materials and Life science Facility in J-PARC

Harada, Masahide; Yamaguchi, Yuji; Kawamura, Seiko; Kofu, Maiko; Nirei, Masami; Haga, Katsuhiro; Oku, Takayuki; Matsuura, Masato*; Kusaka, Katsuhiro*; Nakayama, Haruki*

no journal, , 

In the Materials and Life science experimental Facility (MLF) at J-PARC, 3 GeV proton beam is injected into a mercury target to provide neutrons produced by spallation reactions to neutron instruments, and as of June 2023, MLF is operating at 800 kW proton beam output. The intensity of neutrons provided to the neutron instruments is an important factor to characterize the performance of the neutron instruments. So far, neutron intensity measurements have been done with He-3 counters and gold foil activation methods. To measure both spatial distribution and absolute value simultaneously with high accuracy was an issue. To solve this issue, we proposed the large-area gold-foil activation method for thermal neutrons. In this presentation, we will explain the method of the large-area gold foil activation method and report examples of its application to neutron intensity and distribution measurements at BL02, BL03, and BL14.

Oral presentation

Development of boron-containing Al-based thermal neutron absorber for MW class neutron source

Okutomi, Toshifumi*; Teshigawara, Makoto; Harada, Masahide; Oi, Motoki; Yamaguchi, Yuji; Kuramoto, Shigeru*

no journal, , 

Silver/gold-indium-cadmium (Ag/Au-In-Cd) alloys as thermal neutron absorbers, which can realize high neutron cut-off energy by combining materials with neutron resonance absorption, have been used at the high-intense spallation neutron source in J-PARC. Recently, it has become difficult to treat materials including Cd. We again focused on boron ($$^{10}$$B) having the 1/v absorption and expecting a high neutron cut-off energy as a new thermal neutron absorber. As helium (He) produced by the $$^{10}$$B(n,$$alpha$$) $$^{7}$$Li reaction causes embrittlement of material including $$^{10}$$B, it was considered that the use of $$^{10}$$B was difficult at the high-intense spallation neutron source. Therefore, we have proposed the concept called pre-decoupling, in which other thermal neutron absorber without the He production such as gadolinium (Gd) is combined with $$^{10}$$B in order to suppress the neutron absorption of $$^{10}$$B resulting reducing embrittlement. Based on the pre-decoupling concept, we have developed a material dispersing boron carbide (B$$_{4}$$C) and gadolinium oxide (Gd$$_{2}$$O$$_{3}$$) in aluminum (Al) as a base material. In this presentation, we will report tensile test results of the dispersing materials powder-sintered and the vision of the development.

Oral presentation

Measurement of yield of radionuclides produced by nuclear capture of negative muons

Yamaguchi, Yuji; Niikura, Megumi*; Mizuno, Rurie*; Tampo, Motonobu*; Harada, Masahide; Kawamura, Naritoshi*; Umegaki, Izumi*; Takeshita, Soshi*; Haga, Katsuhiro

no journal, , 

The yield of radionuclides produced by nuclear capture of negative muons has been measured at Muon Science Establishment of Materials and Life Science Experimental Facility (MLF) to accurately estimate radioactivity of muon-irradiated samples at MLF, J-PARC. In this measurement, new data which were difficult to measure at preliminary experiment last year have been obtained by improving the negative-muon counting method.

Oral presentation

Life cycle of the proton beam window in J-PARC MLF

Oi, Motoki; Yamaguchi, Yuji; Kinoshita, Hidetaka; Meigo, Shinichiro; Haga, Katsuhiro

no journal, , 

Material and Life science experimental facility (MLF) in J-PARC is a spallation neutron source which uses 3 GeV proton beam with 1 MW power. The neutron production target is made with mercury and the target vessel is installed in the helium vessel. On the other hands, proton beam transport line is kept in high vacuum, less than 10$$^{-5}$$ Pa to reduce the beam loss. As a boundary of the helium atmosphere and the vacuum region, proton beam window (PBW) is installed. The proton beam window is made with aluminum alloy. Due to the radiation damage of the window, lifetime of the PBW is estimated 10000 MWh. In this summer maintenance period, we replace from the PBW No. 4 to PBW No. 5. In this presentation, we report about life cycle, the structure and replacement work of the PBW.

24 (Records 1-20 displayed on this page)