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(980) meson decaying into
at
2.4 GeV村松 憲仁*; 土川 雄介; LEPS2 BGOegg Collaboration*; 他61名*
Physical Review C, 107(4), p.L042201_1 - L042201_5, 2023/04
被引用回数:5 パーセンタイル:49.60(Physics, Nuclear)For the first time, differential cross sections and photon beam asymmetries were measured for the reaction
by using a linearly polarized photon beam up to 2.4 GeV and a liquid hydrogen target. The
(980) photoproduction signal was clearly observed owing to the absence of contributions from vector-meson photoproduction. The results indicate the
-channel exchange of vector mesons as a mechanism of the
(980) photoproduction at
approximate to 2.1 GeV, putting constraints on the nature of
(980).
photoproduction off the proton at
= 1.3-2.4 GeV村松 憲仁*; 土川 雄介; LEPS2/BGOegg Collaboration*; 他59名*
Physical Review C, 102(2), p.025201_1 - 025201_10, 2020/08
被引用回数:11 パーセンタイル:65.03(Physics, Nuclear)For the reaction
, differential cross sections, photon beam asymmetries, and spin density matrix elements have been measured in the BGOegg experiment at the SPring-8 LEPS2 beamline by using a large acceptance electromagnetic calorimeter. A 1.3-2.4 GeV photon beam with high linear polarization has enabled a precision measurement of photon beam asymmetries
and polarized spin density matrix elements
over a wide angular range, especially above the total energy of about 2 GeV for the first time. The measured
indicates the dominance of
-channel resonances even at higher energies. The
values at backward angles are not reproduced by the existing partial-wave analysis in the highest-energy region, providing new constraints to the contribution of nucleon resonances with high spins.
scattering length from
photoproduction on the proton near the reaction threshold石川 貴嗣*; 藤村 寿子*; 深澤 宏司*; 橋本 亮*; He, Q.*; 本多 佑記*; 保坂 淳; 岩田 高広*; 甲斐田 俊*; 笠木 治郎太*; et al.
Physical Review C, 101(5), p.052201_1 - 052201_6, 2020/05
被引用回数:9 パーセンタイル:53.37(Physics, Nuclear)Photoproduction of the omega meson on the proton has been experimentally studied near the threshold. The total cross sections are determined at incident energies ranging from 1.09 to 1.15 GeV. The 1/2 and 3/2 spin-averaged scattering length 
and effective range 
between the CO meson and proton are estimated from the shape of the total cross section as a function of the incident photon energy: 
= (-0.97
+
(0.07
) fm and 
= (+2.78
) +
(-0.01
) fm, resulting in a repulsive force. The real and imaginary parts for 
and 
are determined separately for the first time. A small
-wave contribution does not affect the obtained values.
(
,
)
and
(
,
)
reactions for 
=1.5-2.4 GeVZegers, R. G. T.*; 住浜 水季*; Ahn, D. S.*; Ahn, J. K.*; 秋宗 秀俊*; 浅野 芳裕; Chang, W. C.*; Dat
, S.*; 江尻 宏泰*; 藤村 寿子*; et al.
Physical Review Letters, 91(9), p.092001_1 - 092001_4, 2003/08
被引用回数:131 パーセンタイル:94.53(Physics, Multidisciplinary)
=1.5-2.4GeVで
(
,
)
,
(
,
)
反応に対するビーム偏極非対称が初めて測定された。この結果は未決定のハドロン共鳴や反応機構解明に用いられる。
= +1 Baryon resonance in photoproduction from the neutron中野 貴志*; Ahn, D. S.*; Ahn, J. K.*; 秋宗 秀俊*; 浅野 芳裕; Chang, W. C.*; 伊達 伸*; 江尻 宏泰*; 藤村 寿子*; 藤原 守; et al.
Physical Review Letters, 91(1), p.012002_1 - 012002_4, 2003/07
被引用回数:1041 パーセンタイル:99.84(Physics, Multidisciplinary)
と
の両粒子を前方で測定することにより、
Cを標的にした
n

n光反応を研究した。1.54GeV/C
に25MeV/C
以下の幅の鋭いバリオン共鳴ピークを観測した。この共鳴ピークのストレンジネス(
)は+1であった。この状態は5つのクォーク(
)が
と中性子に崩壊した状態であると解釈される。