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Entry No. D1932

Y.Kondo1, T.Nakamura1, N.Aoi2, H.Baba3, D.Bazin4, N.Fukuda2, T.Gomi2, H.Hasegawa5, N.Imai2, M.Ishihara2, T.Kobayashi6, T.Kubo2, M.Miura1, T.Motobayashi2, A.Saito3, H.Sakurai7, S.Shimoura3, T.Sugimoto1, K.Watanabe6, Y.X.Watanabe8, T.Yakushiji6, Y.Yanagisawa2, K.Yoneda4
Tokyo Inst.of Technology, Tokyo1
Inst.of Physical and Chemical Res. (RIKEN2
Univ. of Tokyo, Tokyo3
Michigan State University, East Lansing, MI4
error5
Tohoku Univ., Sendai6
Univ. of Tokyo, Tokyo7
High Energy Accelerator Res. Org. (KEK8
Physical Review, Part C, Nuclear Physics71(2005)044611

In-beam gamma-ray spectroscopy of neutron-rich boron isotopes 15,17B via inelastic scattering on 12C

Click on the data number to see the plot. Or select the box to plot multiple data.
DataFilePhysical quantitiesReaction(s)Energies
1 *THTC DSIGMA/DOMEGA
DSIGMA/DOMEGA: dsigma/dOmega #1; THTC: Scattering angle theta in c.m. system #4		 12C(17B,17B)12C; 72 MEV/A
2 *THTC DSIGMA/DOMEGA28)
DSIGMA/DOMEGA: dsigma/dOmega #1; THTC: Scattering angle theta in c.m. system #4		 12C(15B,15B)12C; 72 MEV/A
3 *INC-ENGY-LAB XSECTN
INC-ENGY-LAB: Incident energy in lab. system #3; XSECTN: Cross section #1		 12C(17B,17B)12C; between 72 and 1.20 MEV/A
4 *INC-ENGY-LAB EXC-ENGY XSECTN42) FLAG43)
EXC-ENGY: Excitation energy (of the final state) #2; INC-ENGY-LAB: Incident energy in lab. system #3; XSECTN: Cross section #1		 12C(15B,15B)12C; 72 MEV/A

28) Effective cross section defined by the yield of the simulation (See Eq. 5 of the reference)
42) Effective cross section is defined by the yield of the the simulation.
43)
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