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松田 洋樹; 明午 伸一郎; 岩元 洋介; 吉田 誠*; 長谷川 勝一; 前川 藤夫; 岩元 大樹; 中本 建志*; 石田 卓*; 牧村 俊助*
Journal of Nuclear Science and Technology, 57(10), p.1141 - 1151, 2020/10
被引用回数：2 パーセンタイル：8.37(Nuclear Science & Technology)加速器駆動型核変換システム(ADS)等の陽子ビーム加速器施設におけるビーム窓などの構造材の損傷評価には、原子当たりの弾き出し数(dpa)が損傷指標として広く用いられる。dpaの評価は弾き出し断面積に基づいて行われるものの、20MeV以上のエネルギー領域の陽子に対する弾き出し断面積の実験データは乏しく、計算モデルの間でも約8倍の差が存在している。このため、弾き出し断面積を実験的に取得するのは計算に用いるモデルの評価のために重要となる。弾き出し断面積の取得のため、J-PARCの加速器施設において、0.4-3GeVにわたる陽子エネルギー領域における銅と鉄の断面積を測定した。弾き出し断面積は、損傷を保持するために極低温に冷却された試料における、陽子ビームに金する抵抗率変化により得ることができる。本測定で得られた実験結果を元に、計算モデルの比較検討を行った。広く用いられているNorgertt-Robinson-Torrens (NRT)モデルは、実験値を3.5倍過大評価することが判明した。一方、近年の分子動力学に基づく非熱的再結合補正(arc)モデルは実験値をよく再現したため、銅と鉄の損傷評価にはarcモデルを使うべきであると結論づけられた。
明午 伸一郎; 松田 洋樹; 岩元 洋介; 吉田 誠*; 長谷川 勝一; 前川 藤夫; 岩元 大樹; 中本 建志*; 石田 卓*; 牧村 俊助*
EPJ Web of Conferences, 239, p.06006_1 - 06006_4, 2020/09
加速器駆動型核変換システム(ADS)では、加速器の真空領域と標的領域の隔壁となるビーム入射窓の開発が重要となる。ビーム窓の損傷評価には、原子当たりの弾き出し数(DPA)が用いられるが、DPAの導出に用いられる弾き出し断面積の実験データは20MeV以上のエネルギー領域の陽子に対しほとんどないため、ADSにおいて重要な0.4
3GeV陽子における弾き出し断面積の測定を開始した。弾き出し断面積は、損傷を維持するため極低温に冷却された試料の陽子入射に伴う抵抗率変化を陽子フルエンスとフランケル対当たりの抵抗率変化で除することにより導出できる。実験はJ-PARCセンターの3GeV陽子シンクロトロン施設で行い、試料には銅を用いた。実験で得られた断面積と一般的に弾き出し断面積の計算に使用されるNRTモデルの計算との比較の結果、NRTモデルの計算は実験を約3倍過大評価することが判明した。
at forward and backward rapidity in 
+, 
l, u, and 
He+Au collisions at 
= 200 GeVAcharya, U.*; 長谷川 勝一; 今井 憲一*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他358名*
Physical Review C, 102(1), p.014902_1 - 014902_23, 2020/07
被引用回数：0 パーセンタイル：100(Physics, Nuclear)Charmonium is a valuable probe in heavy-ion collisions to study the properties of the quark gluon plasma, and is also an interesting probe in small collision systems to study cold nuclear matter effects, which are also present in large collision systems. With the recent observations of collective behavior of produced particles in small system collisions, measurements of the modification of harmonium in small systems have become increasingly relevant. We present the results of measurements at forward and backward rapidity in various small collision systems, 
, Al, Au and HeAu, at =200 GeV. The results are presented in the form of the observable 
, the nuclear modification factor, a measure of the ratio of the invariant yield compared to the scaled yield in collisions. We examine the rapidity, transverse momentum, and collision centrality dependence of nuclear effects on production with different projectile sizes and He, and different target sizes Al and Au. The modification is found to be strongly dependent on the target size, but to be very similar for Au and 
HeAu. However, for 0% - 20% central collisions at backward rapidity, the modification for HeAu is found to be smaller than that for Au, with a mean fit to the ratio of 
(stat)
(syst), possibly indicating final state effects due to the larger projectile size.
Al and Au collisions at 
GeVAidala, C.*; 長谷川 勝一; 今井 憲一*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他297名*
Physical Review C, 101(3), p.034910_1 - 034910_16, 2020/03
被引用回数：2 パーセンタイル：13.44(Physics, Nuclear)The PHENIX experiment has studied nuclear effects in Al and Au collisions at GeV on charged hadron production at forward rapidity (
, -going direction) and backward rapidity (
, 
-going direction). Such effects are quantified by measuring nuclear modification factors as a function of transverse momentum and pseudorapidity in various collision multiplicity selections. In central Al and Au collisions, a suppression (enhancement) is observed at forward (backward) rapidity compared to the binary scaled yields in + collisions. The magnitude of enhancement at backward rapidity is larger in Au collisions than in Al collisions, which have a smaller number of participating nucleons. However, the results at forward rapidity show a similar suppression within uncertainties. The results in the integrated centrality are compared with calculations using nuclear parton distribution functions, which show a reasonable agreement at the forward rapidity but fail to describe the backward rapidity enhancement.
and 
production at forward rapidity in + collisions at 
GeVAcharya, U. A.*; 長谷川 勝一; 今井 憲一*; 永宮 正治*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他353名*
Physical Review D, 101(5), p.052006_1 - 052006_13, 2020/03
被引用回数：0 パーセンタイル：100(Astronomy & Astrophysics)The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the differential cross section, mean transverse momentum, mean transverse momentum squared of inclusive and cross-section ratio of to at forward rapidity in 
collisions at 
GeV via the dimuon decay channel. Comparison is made to inclusive cross sections measured at 
GeV and 2.76 - 13 TeV. The result is also compared to leading-order nonrelativistic QCD calculations coupled to a color-glass-condensate description of the low-
gluons in the proton at low transverse momentum (
) and to next-to-leading order nonrelativistic QCD calculations for the rest of the range. These calculations overestimate the data at low . While consistent with the data within uncertainties above 
GeV/
, the calculations are systematically below the data. The total cross section times the branching ratio is BR 
GeV/) = 54.3 
0.5 (stat) 5.5 (syst) nb.
明午 伸一郎; 松田 洋樹; 岩元 洋介; 吉田 誠*; 長谷川 勝一; 前川 藤夫; 岩元 大樹; 中本 建志*; 石田 卓*; 牧村 俊助*
JPS Conference Proceedings (Internet), 28, p.061004_1 - 061004_6, 2020/02
核変換システム等の陽子加速器施設では、標的や窓等の構造材に関する損傷の評価が重要となる。構造材の損傷評価には、原子あたりの弾き出し数(DPA)が広く用いられており、カスケードモデルに基づく計算で得られた弾き出し断面積に粒子束を乗ずることで得られる。DPAによる損傷評価は広く一般的に用いられているものの、20MeV以上のエネルギー範囲における陽子に対する弾き出し断面積の実験データは十分でなく、計算モデル間で約8倍異なることが報告されており構造材の弾き出し断面積の実験データ取得が重要となる。そこで、我々はJ-PARCセンターの3GeV陽子加速器施設を用い、400MeV以上のエネルギー範囲の陽子の弾き出し断面積の測定を開始した。弾き出し損傷断面積は、冷凍機で極低温(4K)に冷却された試料に陽子ビームを照射し、照射に伴う抵抗率の変化により得ることができる。実験で得られた断面積とPHITSコードに一般的に用いられるNRTモデルを用いて計算した結果、計算は実験を3倍程度過大評価を示した。一方、Nordlund等による最新モデルの結果は実験をよく再現し、これまでのNRTモデルに基づく標的等の弾き出し損傷は過大評価していることが明らかになった。
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.
scattering experiment at J-PARC and the analysis status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.
-ray spectroscopy of an 
-shell hypernucleus, 
FYang, 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.
in nuclei through C
spectrum at 1.8 GeV/ in the J-PARC E05 experiment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.
hypernucleus in the J-PARC E13 experiment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.
, Al, and Au collisions at GeVAidala, C.*; 長谷川 勝一; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他296名*
Physical Review Letters, 123(12), p.122001_1 - 122001_9, 2019/09
被引用回数：2 パーセンタイル：45.7(Physics, Multidisciplinary)We report on the nuclear dependence of transverse single-spin asymmetries (TSSAs) in the production of positively-charged hadrons in polarized 
, 
Al and Au collisions at GeV. The measurements have been performed at forward rapidity (
) over the range of 
GeV
and 
. We observed a positive asymmetry 
for positively-charged hadrons in collisions, and a significantly reduced asymmetry in 
+ collisions. These results reveal a nuclear dependence of charged hadron 
in a regime where perturbative techniques are relevant. These results provide new opportunities to use A collisions as a tool to investigate the rich phenomena behind TSSAs in hadronic collisions and to use TSSA as a new handle in studying small-system collisions.
-hypernuclei at J-PARC; Results and perspective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.
bound state in the 
C
reaction at 1.8 GeV/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.
Adare, A.*; 長谷川 勝一; 今井 憲一; 永宮 正治*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他666名*
Physical Review Letters, 123(2), p.022301_1 - 022301_10, 2019/07
被引用回数：6 パーセンタイル：16.18(Physics, Multidisciplinary)The PHENIX collaboration presents first measurements of low-momentum (
GeV/) direct-photon yields from AuAu collisions at =39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in AuAu collisions at =200. Analyzing the photon yield as a function of the experimental observable 
reveals that the low-momentum (
1,GeV/) direct-photon yield 
is a smooth function of and can be well described as proportional to 
with 
1.25. This new scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and Large Hadron Collider, for centrality selected samples, as well as for different, collision systems. At a given beam energy the scaling also holds for high (,GeV/) but when results from different collision energies are compared, an additional -dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
Au collisions at GeVAdare, A.*; 長谷川 勝一; 今井 憲一; 永宮 正治*; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他451名*
Physical Review C, 99(5), p.054903_1 - 054903_29, 2019/05
被引用回数：4 パーセンタイル：18.92(Physics, Nuclear)We present measurements of azimuthal correlations of charged hadron pairs in GeV AuAu collisions after subtracting an underlying event using a model that includes higher-order azimuthal anisotropy 
, 
, and 
. After subtraction, the away-side (
of the highest transverse-momentum trigger (
GeV/) correlations is suppressed compared to that of correlations measured in collisions. At the lowest associated particle , the away-side shape and yield are modified. These observations are consistent with the scenario of radiative-jet energy loss. For the lowest- trigger correlations, an away-side yield exists and we explore the dependence of the shape of the away-side within the context of an underlying-event model. Correlations are also studied differentially versus event-plane angle 
. The angular correlations show an asymmetry when selecting the sign of the trigger-particle azimuthal angle with respect to the 
event plane. This asymmetry and the measured suppression of the pair yield out of plane is consistent with a path-length-dependent energy loss. No 
dependence can be resolved within experimental uncertainties.
collisions at 
GeVAidala, C.*; 長谷川 勝一; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他296名*
Physical Review D, 99(9), p.092003_1 - 092003_21, 2019/05
被引用回数：1 パーセンタイル：76.5(Astronomy & Astrophysics)Measurements of the differential production of electrons from open-heavy-flavor hadrons with charm- and bottom-quark content in collisions at GeV are presented. The measurements proceed through displaced-vertex analyses of electron tracks from the semileptonic decay of charm and bottom hadrons using the PHENIX silicon-vertex detector. The relative contribution of electrons from bottom decays to inclusive heavy-flavor-electron production is found to be consistent with fixed-order-plus-next-to-leading-log perturbative-QCD calculations within experimental and theoretical uncertainties. These new measurements in collisions provide a precision baseline for comparable forthcoming measurements in AA collisions.
GeV proton-nucleus collisionsAidala, C.*; 長谷川 勝一; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他293名*
Physical Review C, 99(4), p.044912_1 - 044912_10, 2019/04
被引用回数：2 パーセンタイル：63.02(Physics, Nuclear)The PHENIX collaboration has measured high- dihadron correlations in , Al, and Au collisions at GeV. The correlations arise from inter- and intra-jet correlations and thus have sensitivity to nonperturbative effects in both the initial and final states. The distributions of 
, the transverse momentum component of the associated hadron perpendicular to the trigger hadron, are sensitive to initial and final state transverse momenta. These distributions are measured multi-differentially as a function of 
, the longitudinal momentum fraction of the associated hadron with respect to the trigger hadron. The near-side widths, sensitive to fragmentation transverse momentum, show no significant broadening between Au, Al, and . The away-side nonperturbative widths are found to be broadened in Au when compared to ; however, there is no significant broadening in Al compared to collisions. The data also suggest that the away-side broadening is a function of 
, the number of binary nucleon-nucleon collisions, in the interaction. The potential implications of these results with regard to initial and final state transverse momentum broadening and energy loss of partons in a nucleus, among other nuclear effects, are discussed.
pairs from open heavy flavor and Drell-Yan in collisions at GeVAidala, C.*; 長谷川 勝一; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; PHENIX Collaboration*; 他287名*
Physical Review D, 99(7), p.072003_1 - 072003_41, 2019/04
被引用回数：5 パーセンタイル：29.95(Astronomy & Astrophysics)PHENIX reports differential cross sections of pairs from semileptonic heavy-flavor decays and the Drell-Yan production mechanism measured in collisions at GeV at forward and backward rapidity (
). The pairs from 
, 
, and Drell-Yan are separated using a simultaneous fit to unlike- and like-sign muon pair spectra in mass and . The azimuthal opening angle correlation between the muons from and decays and the pair- distributions are compared to distributions generated using 
and 
models, which both include next-to-leading order processes. The measured distributions for pairs from are consistent with calculations. The data presents narrower azimuthal correlations and softer distributions compared to distributions generated from . The data are well described by both models. The extrapolated total cross section for bottom production is 
[b], which is consistent with previous measurements at the Relativistic Heavy Ion Collider in the same system at the same collision energy, and is approximately a factor of two higher than the central value calculated with theoretical models. The measured Drell-Yan cross section is in good agreement with next-to-leading-order quantum-chromodynamics calculations.
