ENTRY E1670 20050914 E032E167000000001 SUBENT E1670001 20050914 E032E167000100001 BIB 15 61 E167000100002 TITLE Isobalic analog state of 11Li E167000100003 AUTHOR (T.Teranishi, S.Shimoura, Y.Ando, M.Hirai, N.Iwasa, E167000100004 T.Kikuchi, S.Moriya, T.Motobayashi, H.Murakami, E167000100005 T.Nakamura, T.Nishio, H.Sakurai, T.Uchibori, E167000100006 Y.Watanabe, Y.Yanagisawa, M.Ishihara) E167000100007 INSTITUTE (2JPNIPC) E167000100008 (2JPNYOK) Department of Physics E167000100009 (2JPNTOK) Department of Physics E167000100010 (2GERGSI) E167000100011 REFERENCE (J,PL/B,407,(2),110,199708) Main reference E167000100012 (J,NP/A,630,(1-2),387,199802) E167000100013 S.Shimoura+, Proceedings of The Sixth International E167000100014 Conference on Nucleus-Nucleus Collisions (Gatlinburg, E167000100015 1997) E167000100016 PART-DET (P) E167000100017 (N) E167000100018 (3-LI-9) E167000100019 INC-SOURCE Beam intensity is 20000 PPS. E167000100020 INC-SPECT EN: at the middle of the target E167000100021 SAMPLE - Target enrichment is unknown. E167000100022 - Physical-form of target is solid. E167000100023 - Target is self supported. E167000100024 METHOD (COINC) Detect 9Li, proton and neutron in coincidence. E167000100025 (TOF) To determine velocities of charged particles and E167000100026 neutrons over the 3.1 m flight path between the E167000100027 target and the hodoscope. E167000100028 FACILITY (PRJFS,2JPNIPC) A primary 18O beam of 100 AMeV E167000100029 bombarded a 9Be target of 1.4 g/cm2 E167000100030 thickness. Reaction products were E167000100031 analyzed by the projectile fragment E167000100032 separator RIPS [T.Kubo et al., Nucl. E167000100033 Instr. Meth. B70(1992)309] to obtain a E167000100034 radioactive 11Li beam. E167000100035 ANALYSIS Invariant mass method E167000100036 DETECTOR (SCIN) To detect decay particles from 11Be. The E167000100037 hodoscope consisted of a 5-mm thick Delta E E167000100038 plane and two 60-mm thick E planes. E167000100039 CORRECTION In the reference data given are not corrected for E167000100040 acceptance. In this work, 11Be*(IAS) decays in two E167000100041 ways: 11Be*(IAS) - larger than 9Li+p+n (direct decay) E167000100042 and 11Be*(IAS) -> 10Li+p ->9Li+p+n (Sequential decay). E167000100043 The author assumed direct decay in the evaluation of E167000100044 acceptance. To avoid ambiguity due to this assumption, E167000100045 authors gave raw data (not corrected by acceptance) in E167000100046 the reference. E167000100047 ADD-RES E1670.004:1-H-1(3-LI-11,4-BE-11)0-NN-1 E167000100048 Energy spectrum (Fermi transition part) E167000100049 See NRDF D1670 DATA,3 for detail. E167000100050 E1670.005:1-H-1(3-LI-11,4-BE-11)0-NN-1 E167000100051 Angular distribution (Fermi transition part) E167000100052 See NRDF D1670 DATA,4 for detail. E167000100053 E1670.006:1-H-1(3-LI-11,4-BE-11)0-NN-1 E167000100054 Excitation energy and width of IAS of 11Li. E167000100055 This is obtained by fitting Fermi part of E167000100056 energy spectrum (Fig.2c) with Gaussian E167000100057 function over the region of 0.4 MeV < Ed < E167000100058 1.6 MeV. Effects of the detector acceptance E167000100059 and the Ed resolution were taken into E167000100060 account in the fitting procedure. E167000100061 See NRDF D1670 DATA,5 for detail. E167000100062 HISTORY (20030818T) Data converted from NRDF D1670 E167000100063 ENDBIB 61 0 E167000100064 COMMON 2 3 E167000100065 EN EN-RSL E167000100066 MEV/A PER-CENT E167000100067 64.0 6.0 E167000100068 ENDCOMMON 3 0 E167000100069 ENDSUBENT 68 0 E167000199999 SUBENT E1670002 20050914 E032E167000200001 BIB 7 27 E167000200002 REACTION (1-H-1(3-LI-11,N)4-BE-11,,IPA/DE,,RAW) E167000200003 Uncorrected for detector acceptance E167000200004 EN-SEC ANG is polar angle between beam and 11Be in laboratory E167000200005 system E167000200006 (E-EXC,4-BE-11) Excitation energy of 11Be. This energy E167000200007 is calculated by E(d) + 20.14 MeV E167000200008 where E(d) is decay energy defined in E167000200009 p112 of the reference and 20.14 MeV is E167000200010 threshold energy for the 9Li + p + n E167000200011 channel [G.Audi, A.H.Wapstra, Nucl. E167000200012 Phys. A 595(1995)409]. E167000200013 MISC-COL (MISC1) Decay energy E(d) defined in p112 of the E167000200014 reference E167000200015 (MISC2) Detector acceptance. True energy spectrum can E167000200016 be obtained by dividing tabulated data by this E167000200017 acceptance. E167000200018 SAMPLE - Chemical-form of target is CH2. (CH2)n and C target E167000200019 are used, C target was used to subtract the E167000200020 contributions of carbon nuclei in the (CH2)n target. E167000200021 - Target-thickness: 191 and 188 mg/cm2 for (CH2)n and E167000200022 C target, respectively. E167000200023 ERR-ANALYS (ERR-S) Statistical uncertainty E167000200024 (ERR-SYS) Mainly due to the uncertainty in neutron E167000200025 detection efficiency E167000200026 STATUS (TABLE) Data (Fig.2(a), p112 in reference) received by E167000200027 e-mail from T.Teranishi (2003.09.17) E167000200028 HISTORY (20050812A) On. REACTION corrected (CP-D/430) E167000200029 ENDBIB 27 0 E167000200030 COMMON 3 3 E167000200031 ANG-MIN ANG-MAX ERR-SYS E167000200032 ADEG ADEG PER-CENT E167000200033 0.0 5.0 10.0 E167000200034 ENDCOMMON 3 0 E167000200035 DATA 5 100 E167000200036 E-EXC MISC1 DATA ERR-S MISC2 E167000200037 MEV MEV MB/MEV MB/MEV NO-DIM E167000200038 20.19 0.05 0.00 0.00 0.030 E167000200039 20.29 0.15 0.02 0.01 0.095 E167000200040 20.39 0.25 -0.04 0.03 0.155 E167000200041 20.49 0.35 0.00 0.05 0.200 E167000200042 20.59 0.45 0.17 0.07 0.236 E167000200043 20.69 0.55 0.30 0.08 0.265 E167000200044 20.79 0.65 0.58 0.10 0.287 E167000200045 20.89 0.75 1.00 0.12 0.306 E167000200046 20.99 0.85 1.29 0.13 0.322 E167000200047 21.09 0.95 1.96 0.16 0.336 E167000200048 21.19 1.05 1.97 0.16 0.347 E167000200049 21.29 1.15 1.83 0.15 0.358 E167000200050 21.39 1.25 1.24 0.13 0.368 E167000200051 21.49 1.35 0.81 0.12 0.376 E167000200052 21.59 1.45 1.10 0.11 0.382 E167000200053 21.69 1.55 0.62 0.10 0.387 E167000200054 21.79 1.65 0.72 0.10 0.391 E167000200055 21.89 1.75 0.68 0.10 0.394 E167000200056 21.99 1.85 0.49 0.09 0.397 E167000200057 22.09 1.95 0.47 0.08 0.398 E167000200058 22.19 2.05 0.39 0.08 0.399 E167000200059 22.29 2.15 0.49 0.09 0.399 E167000200060 22.39 2.25 0.48 0.09 0.398 E167000200061 22.49 2.35 0.24 0.07 0.396 E167000200062 22.59 2.45 0.42 0.08 0.394 E167000200063 22.69 2.55 0.28 0.08 0.392 E167000200064 22.79 2.65 0.38 0.07 0.388 E167000200065 22.89 2.75 0.30 0.08 0.384 E167000200066 22.99 2.85 0.15 0.07 0.380 E167000200067 23.09 2.95 0.24 0.07 0.374 E167000200068 23.19 3.05 0.26 0.08 0.369 E167000200069 23.29 3.15 0.33 0.07 0.364 E167000200070 23.39 3.25 0.30 0.07 0.358 E167000200071 23.49 3.35 0.33 0.06 0.351 E167000200072 23.59 3.45 0.23 0.06 0.344 E167000200073 23.69 3.55 0.26 0.07 0.338 E167000200074 23.79 3.65 0.09 0.06 0.331 E167000200075 23.89 3.75 0.09 0.06 0.324 E167000200076 23.99 3.85 0.13 0.06 0.317 E167000200077 24.09 3.95 0.11 0.06 0.309 E167000200078 24.19 4.05 0.15 0.06 0.303 E167000200079 24.29 4.15 0.22 0.06 0.295 E167000200080 24.39 4.25 0.09 0.06 0.287 E167000200081 24.49 4.35 0.18 0.05 0.280 E167000200082 24.59 4.45 0.14 0.06 0.273 E167000200083 24.69 4.55 0.09 0.05 0.266 E167000200084 24.79 4.65 0.19 0.05 0.259 E167000200085 24.89 4.75 0.12 0.05 0.252 E167000200086 24.99 4.85 0.13 0.05 0.245 E167000200087 25.09 4.95 0.10 0.04 0.238 E167000200088 25.19 5.05 0.17 0.05 0.232 E167000200089 25.29 5.15 0.02 0.04 0.225 E167000200090 25.39 5.25 0.04 0.03 0.219 E167000200091 25.49 5.35 0.08 0.04 0.213 E167000200092 25.59 5.45 0.07 0.04 0.207 E167000200093 25.69 5.55 0.11 0.04 0.201 E167000200094 25.79 5.65 0.04 0.04 0.195 E167000200095 25.89 5.75 0.10 0.04 0.190 E167000200096 25.99 5.85 0.09 0.04 0.185 E167000200097 26.09 5.95 0.06 0.04 0.180 E167000200098 26.19 6.05 0.06 0.04 0.174 E167000200099 26.29 6.15 0.08 0.04 0.170 E167000200100 26.39 6.25 0.02 0.04 0.165 E167000200101 26.49 6.35 0.09 0.04 0.161 E167000200102 26.59 6.45 0.07 0.04 0.156 E167000200103 26.69 6.55 0.03 0.03 0.152 E167000200104 26.79 6.65 0.07 0.03 0.148 E167000200105 26.89 6.75 0.04 0.03 0.144 E167000200106 26.99 6.85 0.05 0.03 0.141 E167000200107 27.09 6.95 0.06 0.03 0.137 E167000200108 27.19 7.05 0.04 0.03 0.133 E167000200109 27.29 7.15 0.04 0.03 0.130 E167000200110 27.39 7.25 0.00 0.03 0.127 E167000200111 27.49 7.35 0.03 0.03 0.123 E167000200112 27.59 7.45 0.03 0.03 0.120 E167000200113 27.69 7.55 0.03 0.03 0.117 E167000200114 27.79 7.65 0.07 0.03 0.115 E167000200115 27.89 7.75 0.01 0.02 0.112 E167000200116 27.99 7.85 0.02 0.03 0.109 E167000200117 28.09 7.95 0.04 0.02 0.107 E167000200118 28.19 8.05 0.04 0.03 0.104 E167000200119 28.29 8.15 0.02 0.03 0.101 E167000200120 28.39 8.25 0.06 0.03 0.099 E167000200121 28.49 8.35 0.03 0.03 0.097 E167000200122 28.59 8.45 0.02 0.02 0.095 E167000200123 28.69 8.55 0.08 0.03 0.093 E167000200124 28.79 8.65 0.00 0.02 0.091 E167000200125 28.89 8.75 0.01 0.02 0.089 E167000200126 28.99 8.85 0.01 0.02 0.087 E167000200127 29.09 8.95 0.02 0.02 0.085 E167000200128 29.19 9.05 0.04 0.02 0.083 E167000200129 29.29 9.15 0.01 0.02 0.082 E167000200130 29.39 9.25 0.00 0.02 0.080 E167000200131 29.49 9.35 -0.01 0.03 0.078 E167000200132 29.59 9.45 -0.01 0.02 0.077 E167000200133 29.69 9.55 0.02 0.02 0.075 E167000200134 29.79 9.65 -0.02 0.02 0.074 E167000200135 29.89 9.75 0.02 0.02 0.072 E167000200136 29.99 9.85 0.03 0.02 0.071 E167000200137 30.09 9.95 0.02 0.02 0.069 E167000200138 ENDDATA 102 0 E167000200139 ENDSUBENT 138 0 E167000299999 SUBENT E1670003 20050914 E032E167000300001 BIB 7 27 E167000300002 REACTION (1-H-2(3-LI-11,2N)4-BE-11,,IPA/DE,,RAW) E167000300003 Uncorrected for detector acceptance E167000300004 EN-SEC ANG is polar angle between beam and 11Be in laboratory E167000300005 system E167000300006 (E-EXC,4-BE-11) Excitation energy of 11Be. This energy E167000300007 is calculated by E(d) + 20.14 MeV E167000300008 where E(d) is decay energy defined in E167000300009 p112 of the reference and 20.14 MeV is E167000300010 threshold energy for the 9Li + p + n E167000300011 channel [G.Audi, A.H.Wapstra, Nucl. E167000300012 Phys. A 595(1995)409]. E167000300013 MISC-COL (MISC1) Decay energy E(d) defined in p112 of the E167000300014 reference E167000300015 (MISC2) Detector acceptance. True energy spectrum can E167000300016 be obtained by dividing tabulated data by this E167000300017 acceptance. E167000300018 SAMPLE - Chemical-form of target is CD2. (CD2)n and C target E167000300019 are used, C target was used to subtract the E167000300020 contributions of carbon nuclei in the (CH2)n target. E167000300021 - Target-thickness: 206 and 188 mg/cm2 for (CD2)n and E167000300022 C target, respectively. E167000300023 ERR-ANALYS (ERR-S) Statistical uncertainty E167000300024 (ERR-SYS) Mainly due to the uncertainty in neutron E167000300025 detection efficiency E167000300026 STATUS (TABLE) Data (Fig.2(b), p112 in reference) received by E167000300027 e-mail from T.Teranishi (2003.09.17) E167000300028 HISTORY (20050812A) On. REACTION corrected (CP-D/430) E167000300029 ENDBIB 27 0 E167000300030 COMMON 3 3 E167000300031 ANG-MIN ANG-MAX ERR-SYS E167000300032 ADEG ADEG PER-CENT E167000300033 0.0 5.0 10.0 E167000300034 ENDCOMMON 3 0 E167000300035 DATA 5 100 E167000300036 E-EXC MISC1 DATA ERR-S MISC2 E167000300037 MEV MEV MB/MEV MB/MEV NO-DIM E167000300038 20.19 0.05 0.00 0.00 0.030 E167000300039 20.29 0.15 0.03 0.01 0.095 E167000300040 20.39 0.25 -0.03 0.03 0.155 E167000300041 20.49 0.35 -0.04 0.05 0.200 E167000300042 20.59 0.45 0.04 0.06 0.236 E167000300043 20.69 0.55 0.14 0.07 0.265 E167000300044 20.79 0.65 0.25 0.08 0.287 E167000300045 20.89 0.75 0.51 0.10 0.306 E167000300046 20.99 0.85 0.72 0.11 0.322 E167000300047 21.09 0.95 0.73 0.12 0.336 E167000300048 21.19 1.05 0.67 0.12 0.347 E167000300049 21.29 1.15 0.77 0.12 0.358 E167000300050 21.39 1.25 0.60 0.10 0.368 E167000300051 21.49 1.35 0.60 0.10 0.376 E167000300052 21.59 1.45 0.55 0.09 0.382 E167000300053 21.69 1.55 0.50 0.09 0.387 E167000300054 21.79 1.65 0.43 0.09 0.391 E167000300055 21.89 1.75 0.43 0.08 0.394 E167000300056 21.99 1.85 0.43 0.08 0.397 E167000300057 22.09 1.95 0.42 0.07 0.398 E167000300058 22.19 2.05 0.37 0.08 0.399 E167000300059 22.29 2.15 0.22 0.08 0.399 E167000300060 22.39 2.25 0.28 0.07 0.398 E167000300061 22.49 2.35 0.38 0.08 0.396 E167000300062 22.59 2.45 0.32 0.07 0.394 E167000300063 22.69 2.55 0.24 0.07 0.392 E167000300064 22.79 2.65 0.31 0.07 0.388 E167000300065 22.89 2.75 0.23 0.07 0.384 E167000300066 22.99 2.85 0.21 0.07 0.380 E167000300067 23.09 2.95 0.20 0.07 0.374 E167000300068 23.19 3.05 0.14 0.07 0.369 E167000300069 23.29 3.15 0.23 0.06 0.364 E167000300070 23.39 3.25 0.11 0.06 0.358 E167000300071 23.49 3.35 0.32 0.06 0.351 E167000300072 23.59 3.45 0.30 0.06 0.344 E167000300073 23.69 3.55 0.16 0.06 0.338 E167000300074 23.79 3.65 0.12 0.06 0.331 E167000300075 23.89 3.75 0.19 0.06 0.324 E167000300076 23.99 3.85 0.21 0.06 0.317 E167000300077 24.09 3.95 0.14 0.06 0.309 E167000300078 24.19 4.05 0.18 0.06 0.303 E167000300079 24.29 4.15 0.24 0.05 0.295 E167000300080 24.39 4.25 0.08 0.05 0.287 E167000300081 24.49 4.35 0.09 0.05 0.280 E167000300082 24.59 4.45 0.12 0.05 0.273 E167000300083 24.69 4.55 0.21 0.05 0.266 E167000300084 24.79 4.65 0.16 0.04 0.259 E167000300085 24.89 4.75 0.07 0.05 0.252 E167000300086 24.99 4.85 0.18 0.05 0.245 E167000300087 25.09 4.95 0.17 0.05 0.238 E167000300088 25.19 5.05 0.11 0.05 0.232 E167000300089 25.29 5.15 0.13 0.05 0.225 E167000300090 25.39 5.25 0.13 0.04 0.219 E167000300091 25.49 5.35 0.09 0.04 0.213 E167000300092 25.59 5.45 0.19 0.05 0.207 E167000300093 25.69 5.55 0.11 0.04 0.201 E167000300094 25.79 5.65 0.09 0.04 0.195 E167000300095 25.89 5.75 0.09 0.04 0.190 E167000300096 25.99 5.85 0.05 0.04 0.185 E167000300097 26.09 5.95 0.08 0.04 0.180 E167000300098 26.19 6.05 0.09 0.04 0.174 E167000300099 26.29 6.15 0.09 0.04 0.170 E167000300100 26.39 6.25 0.04 0.04 0.165 E167000300101 26.49 6.35 0.05 0.03 0.161 E167000300102 26.59 6.45 0.09 0.04 0.156 E167000300103 26.69 6.55 0.09 0.04 0.152 E167000300104 26.79 6.65 0.08 0.03 0.148 E167000300105 26.89 6.75 0.07 0.04 0.144 E167000300106 26.99 6.85 0.08 0.04 0.141 E167000300107 27.09 6.95 0.03 0.03 0.137 E167000300108 27.19 7.05 0.12 0.04 0.133 E167000300109 27.29 7.15 0.10 0.03 0.130 E167000300110 27.39 7.25 0.08 0.04 0.127 E167000300111 27.49 7.35 0.05 0.03 0.123 E167000300112 27.59 7.45 0.05 0.03 0.120 E167000300113 27.69 7.55 0.01 0.03 0.117 E167000300114 27.79 7.65 0.09 0.03 0.115 E167000300115 27.89 7.75 0.02 0.03 0.112 E167000300116 27.99 7.85 0.05 0.03 0.109 E167000300117 28.09 7.95 0.10 0.03 0.107 E167000300118 28.19 8.05 0.04 0.03 0.104 E167000300119 28.29 8.15 0.07 0.03 0.101 E167000300120 28.39 8.25 0.04 0.03 0.099 E167000300121 28.49 8.35 0.02 0.02 0.097 E167000300122 28.59 8.45 0.03 0.02 0.095 E167000300123 28.69 8.55 0.05 0.03 0.093 E167000300124 28.79 8.65 0.01 0.02 0.091 E167000300125 28.89 8.75 0.09 0.03 0.089 E167000300126 28.99 8.85 0.03 0.02 0.087 E167000300127 29.09 8.95 0.03 0.02 0.085 E167000300128 29.19 9.05 0.04 0.02 0.083 E167000300129 29.29 9.15 0.00 0.02 0.082 E167000300130 29.39 9.25 -0.02 0.02 0.080 E167000300131 29.49 9.35 0.03 0.03 0.078 E167000300132 29.59 9.45 0.01 0.02 0.077 E167000300133 29.69 9.55 0.04 0.02 0.075 E167000300134 29.79 9.65 0.02 0.02 0.074 E167000300135 29.89 9.75 0.06 0.02 0.072 E167000300136 29.99 9.85 0.07 0.03 0.071 E167000300137 30.09 9.95 0.01 0.02 0.069 E167000300138 ENDDATA 102 0 E167000300139 ENDSUBENT 138 0 E167000399999 NOSUBENT E1670004 20040311 0000E167000400001 NOSUBENT E1670005 20040311 0000E167000500001 NOSUBENT E1670006 20040311 0000E167000600001 ENDENTRY 6 0 E167099999999