Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Jung, W.*; Ahn, J. K.*; 長谷川 勝一; Hicks, K.*; Hwang, S.*; 市川 裕大; Kim, S.*; 佐甲 博之; 佐藤 進; 谷田 聖
JPS Conference Proceedings (Internet), 27, p.011007_1 - 011007_6, 2019/11
We have developed HypTPC consists of TPC and the trigger hodoscope for the J-PARC hadron experiments. The TPC Hodoscope has large scintillators of 80 7
1 cm
to cover the TPC. Especially, we have developed a readout circuit for multiple MPPCs to detect photons generated over a large area of the scintillator. A general methods of applying voltage to multiple MPPCs are parallel and series connections. In the case of parallel connections, a signal has a long tail due to the large sensor capacitance. MEG collaboration used four MPPC segments as a serial connection. However, in the case of a series connection, the requiring bias voltage is very high, and the gain is low. To avoid this problem, we have developed a new individual biasing method with a summing amplifier for stable multiple MPPC readouts. We also made prototype detectors and performed a cosmic-ray test. Brief descriptions of our prototypes and preliminary results of the cosmic-ray test are presented in this article.
中田 祥之*; 長谷川 勝一; 早川 修平*; 細見 健二; 市川 裕大; 今井 憲一; 七村 拓野*; 成木 恵*; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 26, p.023024_1 - 023024_5, 2019/11
J-PARC E40 aims to measure the differential cross sections of the elastic scatterings and the
conversion. A clear peak of
was observed in a missing mass spectrum of the
reaction and recoil protons from the
elastic scattering were successfully observed in the data taken in the summer 2018. The rest of data taking is coming in the spring 2019.
Yang, S. B.*; 長谷川 勝一; 早川 修平*; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 田村 裕和*; 谷田 聖; et al.
JPS Conference Proceedings (Internet), 26, p.023015_1 - 023015_5, 2019/11
We performed a gamma-ray spectroscopy of at J-PARC Hadron Experimental Facility in 2015. It is the first measurement of
rays emitted from
-shell hypernuclei. In this experiment, we determined the energy spacing between the ground state spin doublet,
and
states, as 316 keV. The excitation energies of
and
states are also determined to be 895 and 1266 keV, respectively. The energy spacing is found to be well reproduced by shell-model calculations which describe
- and
-shell
hypernuclei well. The results show that the present theories of the
interaction describe not only the light hypernuclei but also a heavier hypernucleus.
本多 良太郎*; 長谷川 勝一; 早川 修平; 細見 健二; 今井 憲一; 市川 裕大; 七村 拓野; 成木 恵; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 26, p.023014_1 - 023014_4, 2019/11
We measured the reaction spectra at 1.8 GeV/
for the graphite and the polyethylene targets in the J-PARC E05 pilot experiment. By comparing the spectra for these two targets, it was found that
in the
B nucleus is quite broadened. Furthermore, we also compared broadness of
with
obtained in the
spectrum.
seems to be much more broadened in nuclei than
. We gave a possible interpretation, which is related to compositeness of decuplet baryons, for this situation.
中川 真菜美*; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 田村 裕和; 谷田 聖; et al.
JPS Conference Proceedings (Internet), 26, p.023005_1 - 023005_3, 2019/11
The interaction is not much studied than the
interaction. To understand the
interaction, we study
hypernuclei. As for the
hypernucleus, only the ground state of
has been observed. To obtain more information about the
interaction, the excited state should be studied. Therefore, we measure the missing-mass of the
He
reaction at
GeV/
and
2-14
at the J-PARC K1.8 beam line. The ground state of
is observed whereas a peak of the excited states is not observed. We also observe suppression of the
quasi-free process at smaller angles.
Kim, S. H.*; 市川 裕大; 佐甲 博之; 長谷川 勝一; 早川 修平*; 七村 拓野*; 佐藤 進; 谷田 聖; 吉田 純也; 他11名*
Nuclear Instruments and Methods in Physics Research A, 940, p.359 - 370, 2019/10
被引用回数:2 パーセンタイル:34.3(Instruments & Instrumentation)We have developed a gas electron multiplier (GEM)-based time projection chamber (TPC) for the H-dibaryon search experiment at J-PARC. High-rate beam particles enter a TPC gas volume of approximately 0.2 m
, in a direction perpendicular to the electric field. A long-rectangular hollow section is located inside the TPC volume to accommodate a diamond target. We commissioned the TPC using 230 MeV protons with beam rates of up to 1 MHz. The TPC data acquisition system collected 5768 pad signals in full readout mode, with almost 100% efficiency, at a preset trigger rate of 230 Hz. We operated the TPC in an Ar/CH
gas mixture (90/10) without a magnetic field. The spatial resolutions on the pad plane are measured to be 400-700
m, which correspond to 230-300
m in a magnetic field of 1 T. We confirmed high tracking capability at beam rates of up to 1 MHz.
小池 武志*; 長谷川 勝一; 早川 修平*; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 杉村 仁志; 田村 裕和; et al.
AIP Conference Proceedings 2130, p.020011_1 - 020011_9, 2019/07
被引用回数:0 パーセンタイル:100Experimental results from the J-PARC E13 experiments are summarized. A new experimental set up of E13 has established a platform for the future -ray hypernuclear spectroscopy at J-PARC using kaon beams. New
rays are identified in
He and
F. The energy of 1.406 MeV for the
He
transition confirmed a sizable effect of Charge Symmetry Breaking (CSB) in
interaction in the
hypernuclear system. The identification of four
rays in
F is made for the first time in
shell hypernuclei. Especially, energy spacing of the ground state doublet is found to be 315.5 keV. A good agreement with two theoretical calculations suggests that the theoretical formalism used in
shell hypernuclei is also applicable to heavier hypernuclei. Lastly, an overview of the future J-PARC E63 experiment is given.
永江 知文*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 金原 慎二; 七村 拓野*; 成木 恵; et al.
AIP Conference Proceedings 2130, p.020015_1 - 020015_9, 2019/07
For the full understanding of baryon-baryon interactions in flavor , the
interaction is the last missing piece of information. So far, we have revealed the
interaction to be attractive (
MeV), and
interaction to be repulsive in the medium to heavy mass-number region. The
bonding energy is weakly attractive. While we have a few experimental observations suggesting the
interaction would be attractive, there still exist large theoretical ambiguities weather it is attractive or not. Experimental determinations on the existence of bound states of
hypernuclei by observing bound-state peaks are strongly awaited. In this report, a new preliminary result on the missing-mass spectrum of a
C
reaction, which strongly suggests the existence of
-hypernuclear bound states, is presented.
江川 弘行; 足利 沙希子; 長谷川 勝一; 橋本 直; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 金原 慎二*; 七村 拓野; et al.
Progress of Theoretical and Experimental Physics (Internet), 2019(2), p.021D02_1 - 021D02_11, 2019/02
被引用回数:1 パーセンタイル:100(Physics, Multidisciplinary)A double- hypernucleus,
, was observed by the J-PARC E07 collaborationin nuclear emulsions tagged by the
reaction. This event was interpreted as a production and decay of
,
, or
via
capture in
.By assuming the capture in the atomic 3D state, the binding energy of two
hyperons
(
)of these double-
hypernuclei are obtained to be
,
, and
, respectively. Based on the kinematic fitting,
is the most likely explanation for the observed event.
Yang, S. B.*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; et al.
Physical Review Letters, 120(13), p.132505_1 - 132505_5, 2018/03
被引用回数:5 パーセンタイル:35.7(Physics, Multidisciplinary)We report on the first observation of rays emitted from an
-shell hypernucleus,
F. The energy spacing between the ground state doublet,
and
states, of
F is determined to be
keV by measuring the
-ray energy of the
transition. In addition, three
-ray peaks are observed and assigned as
,
, and
transitions. The excitation energies of the
and
states are determined to be
keV and
keV, respectively. It is found that the ground state doublet spacing is well described by theoretical models based on existing
- and
-shell hypernuclear data.
後神 利志*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; 今井 憲一; 市川 裕大; 七村 拓野; 成木 恵; 佐甲 博之; et al.
JPS Conference Proceedings (Internet), 18, p.011031_1 - 011031_6, 2017/11
The missing mass spectroscopy of hypernuclei is planned at the Japan Proton Accelerator Research Complex (J-PARC) by using the
reaction. We are constructing a new magnetic spectrometer, S-2S, which has a better momentum resolution [
(FHWM)] than that of an existing spectrometer (SKS) at J-PARC. S-2S would give us an opportunity to confirm the existence of
hypernuclei as a peak structure owing to both the high momentum resolution and its reasonably large solid angle. Brief descriptions of our experiment and of its preparation status are presentedin this article.
田村 裕和*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 17, p.011004_1 - 011004_11, 2017/07
The present status and future prospects of precision -ray spectroscopy of
hypernuclei are described. A new experiment (J-PARC E13) has been performed at the J-PARC K1.8 line employing a newly-developed germanium (Ge) detector array, Hyperball-J, via the
reaction on
He and
F targets. This is the first study of
-shell and
-shell
hypernuclei with Ge detectors. The
He target spectrum exhibited a
-ray peak of
at
MeV. Compared with the energy (
MeV) of the corresponding transition for the mirror hypernucleus,
, the present result clearly indicates a large charge symmetry breaking (CSB) effect. This decisive data for CSB allows a stringent test of baryon-baryon interaction models. As for the
F target run, a preliminary spectrum shows several
-ray peaks assigned to
transitions. Future plans of
-ray spectroscopy are also discussed.
中川 真菜美*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 17, p.012009_1 - 012009_4, 2017/07
One of the main items of the J-PARC E13 experiment is the search for excited states of the He hypernucleus via the
He
reaction at 1.5 GeV/c. The missing-mass spectrum of the
He
reaction was obtained in an angular range from 0 to 20 degrees. We show the count-base spectrum of the missing-mass in the angular range from 2 to 14 degrees. The ground state of
He and
He were clearly observed in the missing-mass spectrum. We also show three missing-mass spectra divided by the reaction angle.
Yang, S. B.*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 17, p.012004_1 - 012004_4, 2017/07
The first -ray spectroscopy of
-shell hypernucleus,
F, is performed in June, 2015 at the J-PARC K1.8 beam line (J-PARC E13). Precise energy levels of
F can be revealed by measured
rays in this experiment. Especially, the strength of
spin-spin interaction in
-shell hypernucleus is obtained through the energy spacing of the ground-state doublet of the hypernucleus. By comparing its strength between the
,
, and
-shell hypernuclei, a radial dependence
interaction is investigated. The hypernucleus is produced through the
reaction with the beam momentum of 1.8 GeV/c. In very preliminary results, we observed two
rays, and their energies are
keV and
keV where the uncertainties are only statistical.
本多 良太郎*; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 永宮 正治; 佐甲 博之; 佐藤 進; 杉村 仁志; et al.
Physical Review C, 96(1), p.014005_1 - 014005_23, 2017/07
被引用回数:9 パーセンタイル:22.36(Physics, Nuclear)We searched for the bound state of the neutron-rich -hypernucleus
H, using the
Li
double charge-exchange reaction at a
beam momentum of 1.2 GeV/
at J-PARC. A total of
was driven onto a
Li target of 3.5 g/cm
thickness. No event was observed below the bound threshold, i.e., the mass of
H+
, in the missing-mass spectrum of the
Li
reaction in the
angular range. Furthermore, no event was found up to 2.8 MeV/c
above the bound threshold.
佐甲 博之; 長谷川 勝一; 細見 健二; 市川 裕大; 今井 憲一; Hicks, K.*; Ahn, J. K.*; Kim, S. H.*; Lee, J. W.*; Hwang, S. H.*
Proceedings of Science (Internet), 5 Pages, 2017/05
バリオン励起状態(N,
)は長年にわたって研究されてきたが、その性質や質量スペクトルに関する我々の知見は大変限られている。最近、Dynamical-Couple Channel (DCC)模型の発展により、
反応がこれらの励起状態に大きく寄与することが分かってきた。しかしながら、
反応データは1970年代に測定された24万事象に限られており、決定的に不足している。そのため、我々はJ-PARCにおいて統計を二桁上げるE45実験を提案した。この実験においては、
Hzの
ビームを用いて超電導Helmholtz型双極磁石に設置したTime Projection Chamberでこれらの反応を測定する。これらの測定をビーム運動量を細かく変えながら高統計で測定する。本発表では実験の設計と準備状況、シミュレーションの結果を報告する。
永江 知文*; 江川 弘行; 長谷川 勝一; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 杉村 仁志; 谷田 聖; et al.
Proceedings of Science (Internet), 7 Pages, 2017/05
We have carried out a pilot data taking of the J-PARC E05 experiment to search for the bound state peaks of Be in the
C
reaction at 1.8 GeV/
. The measurement was performed at the K1.8 beam line of the J-PARC hadron experimental hall with a typical
beam intensity of
every six seconds. So far the best energy resolution of about 6 MeV FWHM was achieved with the existing SKS spectrometer. With a reasonable statistics, we have succeeded to observe peak structures in the bound region, which seems to suggest that the potential depth of
would be deeper than 14 MeV estimated in the previous measurements.
市川 正一; 千葉 悠介; 大野 史靖; 羽鳥 雅一; 小林 孝典; 上倉 亮一; 走利 信男*; 犬塚 泰輔*; 北野 寛*; 阿部 恒*
JAEA-Research 2017-001, 40 Pages, 2017/03
日本原子力研究開発機構は、高速増殖原型炉もんじゅのプラント工程への影響を低減するため、現在、原子炉格納容器全体漏えい率試験で用いている塩化リチウム式露点検出器の代替品として、静電容量式露点検出器の検証試験を実施した。原子炉格納容器全体漏えい率試験(試験条件: 窒素雰囲気、24時間)における静電容量式露点検出器の測定結果は、既存の塩化リチウム式検出器と比較して有意な差は無かった。また、長期検証試験(試験条件:空気雰囲気、2年間)においては、静電容量式露点検出器は、高精度鏡面式露点検出器との比較の結果、「電気技術規程(原子力編)」の「原子炉格納容器の漏えい試験規定」に基づく使用前検査時に要求される機器精度(精度:2.04
C)を長期間にわたり有することを確認した。
市川 正一; 千葉 悠介; 大野 史靖; 羽鳥 雅一; 小林 孝典; 上倉 亮一; 走利 信男*; 犬塚 泰輔*; 北野 寛*; 阿部 恒*
JAEA-Research 2016-021, 32 Pages, 2017/02
日本原子力研究開発機構は、高速増殖原型炉もんじゅのプラント工程への影響を低減するため、現在、原子炉格納容器全体漏えい率試験で用いている塩化リチウム式露点検出器の代替品として、静電容量式露点検出器の検証試験を実施した。原子炉格納容器全体漏えい率試験(試験条件: 窒素雰囲気、24時間)における静電容量式露点検出器の測定結果は、既存の塩化リチウム式検出器と比較して有意な差は無かった。また、長期検証試験(試験条件: 空気雰囲気、2年間)においては、静電容量式露点検出器は、高精度鏡面式露点検出器との比較の結果、「電気技術規程(原子力編)」の「原子炉格納容器の漏えい率試験規程」に基づく使用前検査時に要求される機器精度(精度: 2.04
C)を長期間にわたり有することを確認した。
市川 裕大; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; 今井 憲一; 金原 慎二; 中田 祥之; 佐甲 博之; 佐藤 進; et al.
JPS Conference Proceedings (Internet), 13, p.020007_1 - 020007_5, 2017/02
これまで反K中間子と原子核の間の相互作用はK中間子原子(K-中間子と原子核の電磁相互作用による束縛状態)のX線を用いて研究が行われてきた。しかし、このK中間子原子のX線測定では理論モデルの種類によって結果が大きく依存するという問題がため、X線測定だけでは相互作用を決定することが困難である。そこで、われわれはC(K
, p)反応におけるエネルギースペクトルを測定し、理論計算と比較する手法を用いて反K中間子と原子核の間の相互作用を決定しようとしている。この手法は既にKEK E548実験で行われているが、実験セットアップ上の問題点が指摘されているため、過去の高エネルギー加速器研究機構での実験では不十分である。そこで、われわれはJ-PARCにおいて再実験を行い、正しく
C(K
, p)のスペクトルを取得することに成功した。