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Entry No. D1789

H.Noumi1, P.K.Saha1, D.Abe2, S.Ajimura3, K.Aoki1, H.C.Bhang4, T.Endo2, Y.Fujii2, T.Fukuda1, H.C.Guo5, K.Imai7, O.Hashimoto2, H.Hotchi6, E.H.Kim4, J.H.Kim4, T.Kishimoto3, A.Krutenkova8, K.Maeda2, T.Nagae1, M.Nakamura6, H.Outa1, M.Sekimoto1, T.Saito2, A.Sakaguchi3, Y.Sato1,2, R.Sawafta9, Y.Shimizu3, T.Takahashi2, L.Tang10, H.Tamura2, K.Tanida6, T.Watanabe2, H.H.Xia5, S.H.Zhou5, L.H.Zhu7, X.F.Zhu5
High Energy Accelerator Res. Org. (KEK1
Tohoku Univ., Sendai2
Osaka Univ., Osaka3
Natl.Seoul Univ., Seoul4
Inst.of Atomic Energy, Beijing5
Univ. of Tokyo, Tokyo6
Kyoto Univ.7
Inst. Teoret. + Experiment. Fiziki, Moscow8
United States of America9
United States of America10
Physical Review Letters89(2002)072301

Sigma-nucleus potential in A = 28

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DataFilePhysical quantitiesReaction(s)Energies
1 *THTL DSIGMA/DOMEGA18)
DSIGMA/DOMEGA: dsigma/dOmega #1; THTL: Scattering angle theta in lab. system #4		 P(PIN,KP)SIGMAN;
2 *ENGY21) DSIGMA/DOMEGA/DE
DSIGMA/DOMEGA/DE: d2sigma/dOmega/dE #1; ENGY: Energy		 SI(PIN,KP)X;

18) Fig.1 shows that the missing-mass spectrum for hydrogen baryon (m=1197 MeV/c**2).
21) Minus of the Sigma- binding energy (-B(Sigma-))
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Last update of this script: April 12, 2006. Contact address: darpe-admin@jcprg.org