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Entry No. D1670

T.Teranishi1, S.Shimoura2, Y.Ando2, M.Hirai3, N.Iwasa2, T.Kikuchi2, S.Moriya2, T.Motobayashi2, H.Murakami2, T.Nakamura3, T.Nishio2, H.Sakurai1, T.Uchibori2, Y.Watanabe1, Y.Yanagisawa2, M.Ishihara1,3
Inst.of Physical and Chemical Res. (RIKEN1
error2
Univ. of Tokyo, Tokyo3
Gesellschaft fuer Schwerionenforschung, Darmstadt4
error(407(1997)110'5')

Isobalic analog state of 11Li

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DataFilePhysical quantitiesReaction(s)Energies
1 *EXC-ENGY-EMT16) DATA117) DSIGMA/DE18) DATA220)
DSIGMA/DE: dsigma/dE #1; EXC-ENGY-EMT: Excitation energy of outgoing particle #2		 P(11LI,11BE)N; 64 MEV/A
2 *EXC-ENGY-EMT24) DATA125) DSIGMA/DE26) DATA228)
DSIGMA/DE: dsigma/dE #1; EXC-ENGY-EMT: Excitation energy of outgoing particle #2		 D(11LI,11BE)N; 64 MEV/A
3 *EXC-ENGY-EMT33) DATA134) DSIGMA/DE35) DATA237)
DSIGMA/DE: dsigma/dE #1; EXC-ENGY-EMT: Excitation energy of outgoing particle #2		 P(11LI,11BE)N; 64 MEV/A
4 *THTL DSIGMA/DOMEGA42) DATA144)
DSIGMA/DOMEGA: dsigma/dOmega #1; THTL: Scattering angle theta in lab. system #4		 P(11LI,11BE)N; 64 MEV/A
5 *EXC-ENGY WDTH
EXC-ENGY: Excitation energy (of the final state) #2; WDTH: Width		 P(11LI,11BE)N; 64 MEV/A

16) Excitation energy of 11Be. This energy is calculated by 595(1995)409].
17) Decay energy E(d) defined in p112 of the reference
18) Uncorrected for detector acceptance
20) Detector acceptance. True energy spectrum can be obtained by dividing tabulated data by this acceptance.
24) Excitation energy of 11Be. This energy is calculated by 595(1995)409].
25) Decay energy E(d) defined in p112 of the reference
26) Uncorrected for detector acceptance
28) Detector acceptance. True energy spectrum can be obtained by dividing tabulated data by this acceptance.
33) Excitation energy of 11Be. This energy is calculated by 595(1995)409].
34) Decay energy E(d) defined in p112 of the reference
35) This spectrum is obtained by subtracting (d,2n) spectrum spectrum. Uncorrected for detector acceptance.
37) Detector acceptance. True energy spectrum can be obtained by dividing tabulated data by this acceptance.
42) This distribution is obtained by subtracting (d,2n) from (p,n) spectrum. Uncorrected for detector acceptance.
44) Detector acceptance. True angular distribution can be obtained by dividing tabulated data by this acceptance.
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Last update of this script: April 12, 2006. Contact address: darpe-admin@jcprg.org