ENTRY C1890 20120517 C118C189000000001 SUBENT C1890001 20120517 C118C189000100001 BIB 8 26 C189000100002 TITLE Resonances in 11C observed in the 4He(7Be,alpha)7Be C189000100003 and 4He(7Be,p)10B reactions C189000100004 AUTHOR (M.Freer,N.L.Achouri,C.Angulo,N.I.Ashwood,D.W.Bardayan,C189000100005 S.Brown,W.N.Catford,K.A.Chipps,N.Curtis,P.Demaret, C189000100006 C.Harlin,B.Laurent,J.D.Malcolm,M.Milin,T.Munoz-Britton,C189000100007 N.A.Orr,S.D.Pain,D.Price,R.Raabe,N.Soic,J.S.Thomas, C189000100008 C.Wheldon,G.Wilson,V.A.Ziman) C189000100009 INSTITUTE (2UK BIR,2FR CAE,2BLGLVN,1USAORL,2UK SUR,3CROZAG, C189000100010 2BLGLEU,3CRORBZ) C189000100011 (1USAUSA)The State University of New Jersey, C189000100012 Piscataway,New Jersey C189000100013 REFERENCE (J,PR/C,85,014304,2012) C189000100014 METHOD The technique of resonance scattering with a thick C189000100015 target was used.It involves the passage of a beam C189000100016 through a target material. As the beam slows down and C189000100017 the center-of-mass energy coincides with that of a C189000100018 resonance of the composite system then a resonant C189000100019 component to the scattering process occurs. Inverse C189000100020 kinematics was used and the resonant decay by C189000100021 light particle emission was observed at zero degrees. C189000100022 INC-SOURCE The 7Be was produced by first irradiating a natural C189000100023 lithium target with a beam of 27-MeV protons and then C189000100024 the 7Be (T1/2 = 53.2 days) was chemically separated C189000100025 and installed into an ion source. C189000100026 ERR-ANALYS (ERR-S) Statistical uncertainty C189000100027 HISTORY (20120517C) Compiled by S.H. C189000100028 ENDBIB 26 0 C189000100029 NOCOMMON 0 0 C189000100030 ENDSUBENT 29 0 C189000199999 SUBENT C1890002 20120517 C118C189000200001 BIB 5 16 C189000200002 REACTION (2-HE-4(4-BE-7,P)5-B-10,,DA) C189000200003 STATUS (TABLE) Data presented in fig. 3 of the reference C189000200004 sent by author (M.F.), LLN data C189000200005 FACILITY (CYCLO,2BLGLVN) First experiment was performed C189000200006 using cyclotron at Louvain-la-Neuve C189000200007 DETECTOR (SISD)The silicon array used for the measurements was C189000200008 housed within the sample gas volume. The array was C189000200009 arranged in a LEDA-type configuration composed of 8 C189000200010 YY1-type silicon strip detectors of thickness 500 C189000200011 mu-m. The plane of the array was placed 69 cm from C189000200012 the entrance window and the detectors covered a range C189000200013 of angles from 4.1. to 10.7. with respect to the C189000200014 chamber window. Time of flight relative to cyclotron C189000200015 frequency was measured. C189000200016 SAMPLE He gas target with length of 69 cm at He pressure C189000200017 of 110 mbar C189000200018 ENDBIB 16 0 C189000200019 COMMON 1 3 C189000200020 ANG C189000200021 ADEG C189000200022 0.0 C189000200023 ENDCOMMON 3 0 C189000200024 DATA 3 47 C189000200025 EN-CM DATA ERR-S C189000200026 MEV MB/SR MB/SR C189000200027 9.01 0.27 0.19 C189000200028 9.02 0.76 0.25 C189000200029 9.03 0.64 0.23 C189000200030 9.05 0.78 0.22 C189000200031 9.06 0.76 0.21 C189000200032 9.08 0.53 0.18 C189000200033 9.09 0.92 0.23 C189000200034 9.11 0.94 0.24 C189000200035 9.12 1.20 0.27 C189000200036 9.13 1.10 0.26 C189000200037 9.15 1.38 0.29 C189000200038 9.16 1.73 0.33 C189000200039 9.18 1.44 0.31 C189000200040 9.19 1.41 0.31 C189000200041 9.21 2.33 0.40 C189000200042 9.23 1.90 0.37 C189000200043 9.24 2.38 0.41 C189000200044 9.26 2.80 0.46 C189000200045 9.27 2.87 0.47 C189000200046 9.29 2.87 0.47 C189000200047 9.30 3.34 0.52 C189000200048 9.32 4.25 0.59 C189000200049 9.33 4.33 0.59 C189000200050 9.35 2.55 0.46 C189000200051 9.37 3.81 0.57 C189000200052 9.38 3.49 0.55 C189000200053 9.40 4.49 0.64 C189000200054 9.42 3.98 0.61 C189000200055 9.43 4.01 0.62 C189000200056 9.45 4.53 0.67 C189000200057 9.47 5.70 0.76 C189000200058 9.48 4.63 0.70 C189000200059 9.50 4.90 0.73 C189000200060 9.52 4.62 0.72 C189000200061 9.53 5.73 0.82 C189000200062 9.55 6.19 0.87 C189000200063 9.57 9.41 1.06 C189000200064 9.59 8.16 1.01 C189000200065 9.60 7.45 0.99 C189000200066 9.62 8.87 1.10 C189000200067 9.64 8.27 1.09 C189000200068 9.66 6.71 1.00 C189000200069 9.67 10.32 1.28 C189000200070 9.69 8.39 1.18 C189000200071 9.71 10.05 1.31 C189000200072 9.73 8.23 1.23 C189000200073 9.75 6.00 1.08 C189000200074 ENDDATA 49 0 C189000200075 ENDSUBENT 74 0 C189000299999 SUBENT C1890003 20120517 C118C189000300001 BIB 5 13 C189000300002 REACTION (2-HE-4(4-BE-7,P)5-B-10,,DA) C189000300003 STATUS (TABLE) Data presented in fig. 3 of the reference C189000300004 sent by author (M.F.) ORNL data C189000300005 FACILITY (VDGT,1USAORL) Second set of measurements was C189000300006 performed using a previously prepared 7Be sample C189000300007 placed in the ion source of the HRIBF tandem C189000300008 accelerator at ORNL C189000300009 DETECTOR (TELES,SI,SI) The Si E-dE telescope was capable of C189000300010 distinguishing protons from heavier elements, i.e. C189000300011 alpha particles. Detectors were calibrated using C189000300012 241Am and 244Cm alpha sources. C189000300013 SAMPLE He gas target with length of 38 cm at He pressure C189000300014 of 920 mbar C189000300015 ENDBIB 13 0 C189000300016 COMMON 1 3 C189000300017 ANG C189000300018 ADEG C189000300019 0.0 C189000300020 ENDCOMMON 3 0 C189000300021 DATA 3 38 C189000300022 EN-CM DATA ERR-S C189000300023 MEV MB/SR MB/SR C189000300024 11.49 1.74 0.58 C189000300025 11.59 3.04 0.78 C189000300026 11.69 5.72 1.10 C189000300027 11.79 6.87 1.23 C189000300028 11.89 4.16 0.98 C189000300029 11.99 6.51 1.25 C189000300030 12.09 10.04 1.59 C189000300031 12.19 7.31 1.38 C189000300032 12.29 7.60 1.44 C189000300033 12.39 12.97 1.91 C189000300034 12.49 10.54 1.76 C189000300035 12.59 6.07 1.36 C189000300036 12.69 3.15 1.00 C189000300037 12.79 3.26 1.03 C189000300038 12.89 2.70 0.95 C189000300039 12.99 4.19 1.21 C189000300040 13.09 3.61 1.14 C189000300041 13.19 2.99 1.06 C189000300042 13.29 5.40 1.44 C189000300043 13.39 4.38 1.32 C189000300044 13.49 2.47 1.01 C189000300045 13.59 2.97 1.12 C189000300046 13.69 3.51 1.24 C189000300047 13.79 4.97 1.50 C189000300048 13.89 3.73 1.32 C189000300049 13.99 5.77 1.66 C189000300050 14.09 3.47 1.31 C189000300051 14.19 6.64 1.84 C189000300052 14.29 3.16 1.29 C189000300053 14.39 2.17 1.08 C189000300054 14.49 3.91 1.48 C189000300055 14.59 1.15 0.81 C189000300056 14.69 1.78 1.03 C189000300057 14.79 0.61 0.61 C189000300058 14.89 1.89 1.09 C189000300059 14.99 0.65 0.65 C189000300060 15.09 0.67 0.67 C189000300061 15.29 1.42 1.00 C189000300062 ENDDATA 40 0 C189000300063 ENDSUBENT 62 0 C189000399999 SUBENT C1890004 20120517 C118C189000400001 BIB 5 16 C189000400002 REACTION (2-HE-4(4-BE-7,EL)2-HE-4,,DA,A) C189000400003 STATUS (TABLE) Data presented in fig. 3 of the reference C189000400004 sent by author (M.F.) LLN data C189000400005 FACILITY (CYCLO,2BLGLVN) First experiment was performed C189000400006 using cyclotron at Louvain-la-Neuve C189000400007 DETECTOR (SISD)The silicon array used for the measurements was C189000400008 housed within the sample gas volume. The array was C189000400009 arranged in a LEDA-type configuration composed of 8 C189000400010 YY1-type silicon strip detectors of thickness 500 C189000400011 mu-m. The plane of the array was placed 69 cm from C189000400012 the entrance window and the detectors covered a range C189000400013 of angles from 4.1. to 10.7. with respect to the C189000400014 chamber window. Time of flight relative to cyclotron C189000400015 frequency was measured. C189000400016 SAMPLE He gas target with length of 69 cm at He pressure C189000400017 of 110 mbar C189000400018 ENDBIB 16 0 C189000400019 COMMON 1 3 C189000400020 ANG C189000400021 ADEG C189000400022 0.0 C189000400023 ENDCOMMON 3 0 C189000400024 DATA 3 107 C189000400025 EN-CM DATA ERR-S C189000400026 MEV MB/SR MB/SR C189000400027 0.72 184.48 8.95 C189000400028 0.74 225.91 10.00 C189000400029 0.75 191.52 6.57 C189000400030 0.76 191.62 4.67 C189000400031 0.77 211.71 3.52 C189000400032 0.79 155.71 2.48 C189000400033 0.80 152.48 2.38 C189000400034 0.81 100.95 1.62 C189000400035 0.83 84.04 1.47 C189000400036 0.84 82.55 1.47 C189000400037 0.85 77.91 1.39 C189000400038 0.87 76.46 1.39 C189000400039 0.88 72.79 1.36 C189000400040 0.89 73.99 1.38 C189000400041 0.91 74.89 1.40 C189000400042 0.92 78.53 1.43 C189000400043 0.93 78.55 1.45 C189000400044 0.94 82.87 1.49 C189000400045 0.96 81.61 1.49 C189000400046 0.97 78.64 1.46 C189000400047 0.98 80.62 1.49 C189000400048 1.00 79.19 1.48 C189000400049 1.01 74.31 1.44 C189000400050 1.02 74.28 1.45 C189000400051 1.03 70.11 1.40 C189000400052 1.05 75.13 1.47 C189000400053 1.06 69.19 1.38 C189000400054 1.07 64.11 1.33 C189000400055 1.09 65.80 1.35 C189000400056 1.10 66.01 1.36 C189000400057 1.11 65.64 1.36 C189000400058 1.13 64.91 1.36 C189000400059 1.14 63.03 1.35 C189000400060 1.15 64.21 1.37 C189000400061 1.17 65.81 1.40 C189000400062 1.18 63.77 1.38 C189000400063 1.19 59.36 1.33 C189000400064 1.20 60.99 1.36 C189000400065 1.22 61.91 1.38 C189000400066 1.23 60.04 1.37 C189000400067 1.24 59.15 1.33 C189000400068 1.26 60.29 1.36 C189000400069 1.27 56.62 1.31 C189000400070 1.28 58.26 1.34 C189000400071 1.30 57.48 1.34 C189000400072 1.31 52.98 1.30 C189000400073 1.32 55.91 1.34 C189000400074 1.34 54.31 1.32 C189000400075 1.35 51.64 1.30 C189000400076 1.36 52.77 1.31 C189000400077 1.37 50.12 1.29 C189000400078 1.39 49.66 1.29 C189000400079 1.40 49.27 1.30 C189000400080 1.41 48.96 1.30 C189000400081 1.43 50.18 1.31 C189000400082 1.44 50.57 1.32 C189000400083 1.45 48.24 1.30 C189000400084 1.47 47.75 1.27 C189000400085 1.48 47.29 1.27 C189000400086 1.49 48.01 1.28 C189000400087 1.50 44.35 1.24 C189000400088 1.52 47.06 1.28 C189000400089 1.53 43.97 1.24 C189000400090 1.54 44.31 1.25 C189000400091 1.56 43.14 1.24 C189000400092 1.57 40.86 1.21 C189000400093 1.58 41.95 1.22 C189000400094 1.59 38.43 1.18 C189000400095 1.61 38.62 1.18 C189000400096 1.62 37.23 1.17 C189000400097 1.64 35.43 1.14 C189000400098 1.65 34.71 1.14 C189000400099 1.66 32.27 1.11 C189000400100 1.67 31.50 1.10 C189000400101 1.69 29.87 1.07 C189000400102 1.70 32.94 1.12 C189000400103 1.71 33.07 1.13 C189000400104 1.73 33.43 1.15 C189000400105 1.74 31.69 1.13 C189000400106 1.75 30.60 1.11 C189000400107 1.76 30.22 1.11 C189000400108 1.78 30.48 1.12 C189000400109 1.79 32.57 1.16 C189000400110 1.80 31.42 1.14 C189000400111 1.82 33.49 1.19 C189000400112 1.83 32.25 1.17 C189000400113 1.84 32.56 1.18 C189000400114 1.86 33.20 1.20 C189000400115 1.87 31.25 1.17 C189000400116 1.88 32.75 1.20 C189000400117 1.90 32.31 1.20 C189000400118 1.91 34.53 1.24 C189000400119 1.92 31.89 1.19 C189000400120 1.93 32.00 1.20 C189000400121 1.95 31.70 1.19 C189000400122 1.96 30.19 1.16 C189000400123 1.97 31.14 1.18 C189000400124 1.99 28.63 1.13 C189000400125 2.00 30.15 1.16 C189000400126 2.01 28.77 1.14 C189000400127 2.02 29.40 1.14 C189000400128 2.04 28.31 1.13 C189000400129 2.05 25.99 1.08 C189000400130 2.07 22.75 1.02 C189000400131 2.08 22.32 1.01 C189000400132 2.09 17.71 0.91 C189000400133 2.10 17.05 0.91 C189000400134 ENDDATA 109 0 C189000400135 ENDSUBENT 134 0 C189000499999 SUBENT C1890005 20120517 C118C189000500001 BIB 5 13 C189000500002 REACTION (2-HE-4(4-BE-7,EL)2-HE-4,,DA,A) C189000500003 STATUS (TABLE) Data presented in fig. 3 of the reference C189000500004 sent by author (M.F.) ORNL data C189000500005 FACILITY (VDGT,1USAORL) Second set of measurements was C189000500006 performed using a previously prepared 7Be sample C189000500007 placed in the ion source of the HRIBF tandem C189000500008 accelerator at ORNL C189000500009 DETECTOR (TELES,SI,SI) The Si E-dE telescope was capable of C189000500010 distinguishing protons from heavier elements, i.e. C189000500011 alpha particles. Detectors were calibrated using C189000500012 241Am and 244Cm alpha sources. C189000500013 SAMPLE He gas target with length of 38 cm at He pressure C189000500014 of 920 mbar C189000500015 ENDBIB 13 0 C189000500016 COMMON 1 3 C189000500017 ANG C189000500018 ADEG C189000500019 0.0 C189000500020 ENDCOMMON 3 0 C189000500021 DATA 3 264 C189000500022 EN-CM DATA ERR-S C189000500023 MEV MB/SR MB/SR C189000500024 1.50 48.62 2.06 C189000500025 1.52 48.14 2.10 C189000500026 1.54 46.09 2.10 C189000500027 1.56 45.48 2.13 C189000500028 1.58 46.01 2.18 C189000500029 1.60 38.15 2.03 C189000500030 1.62 40.51 2.13 C189000500031 1.64 41.21 2.19 C189000500032 1.66 33.31 2.00 C189000500033 1.68 34.85 2.08 C189000500034 1.70 32.30 2.04 C189000500035 1.72 32.56 2.08 C189000500036 1.74 30.86 2.06 C189000500037 1.76 31.96 2.13 C189000500038 1.78 23.01 1.83 C189000500039 1.80 30.89 2.15 C189000500040 1.82 30.69 2.18 C189000500041 1.84 32.03 2.25 C189000500042 1.86 30.62 2.23 C189000500043 1.88 29.93 2.24 C189000500044 1.90 33.80 2.41 C189000500045 1.92 28.68 2.25 C189000500046 1.94 27.77 2.24 C189000500047 1.96 25.31 2.16 C189000500048 1.98 26.29 2.23 C189000500049 2.00 26.90 2.28 C189000500050 2.02 23.56 2.16 C189000500051 2.04 23.68 2.19 C189000500052 2.06 18.83 1.97 C189000500053 2.08 21.14 2.11 C189000500054 2.10 19.64 2.06 C189000500055 2.12 21.16 2.16 C189000500056 2.14 24.07 2.33 C189000500057 2.16 22.49 2.27 C189000500058 2.18 24.57 2.40 C189000500059 2.20 23.38 2.36 C189000500060 2.22 22.37 2.33 C189000500061 2.24 21.06 2.28 C189000500062 2.26 26.25 2.57 C189000500063 2.28 24.93 2.53 C189000500064 2.30 27.21 2.67 C189000500065 2.32 26.63 2.66 C189000500066 2.34 28.18 2.76 C189000500067 2.36 30.05 2.88 C189000500068 2.38 26.92 2.75 C189000500069 2.40 31.36 2.99 C189000500070 2.42 30.14 2.96 C189000500071 2.44 31.82 3.06 C189000500072 2.46 29.64 2.98 C189000500073 2.48 39.84 3.48 C189000500074 2.50 39.85 3.51 C189000500075 2.52 47.69 3.87 C189000500076 2.54 41.10 3.62 C189000500077 2.56 55.31 4.23 C189000500078 2.58 51.55 4.11 C189000500079 2.60 55.31 4.29 C189000500080 2.62 41.93 3.77 C189000500081 2.64 50.08 4.14 C189000500082 2.66 38.62 3.67 C189000500083 2.68 53.29 4.34 C189000500084 2.70 42.95 3.92 C189000500085 2.72 41.73 3.89 C189000500086 2.74 34.58 3.57 C189000500087 2.76 43.63 4.03 C189000500088 2.78 40.44 3.91 C189000500089 2.80 42.13 4.02 C189000500090 2.82 35.71 3.72 C189000500091 2.84 45.22 4.22 C189000500092 2.86 35.85 3.78 C189000500093 2.88 32.28 3.61 C189000500094 2.90 24.11 3.14 C189000500095 2.92 28.14 3.41 C189000500096 2.94 21.79 3.02 C189000500097 2.96 17.82 2.75 C189000500098 2.98 15.89 2.61 C189000500099 3.00 14.78 2.53 C189000500100 3.02 14.08 2.49 C189000500101 3.04 15.58 2.63 C189000500102 3.06 9.91 2.11 C189000500103 3.08 12.31 2.37 C189000500104 3.10 12.45 2.40 C189000500105 3.12 13.06 2.47 C189000500106 3.14 12.27 2.41 C189000500107 3.16 12.41 2.43 C189000500108 3.18 11.10 2.32 C189000500109 3.20 15.62 2.76 C189000500110 3.22 10.37 2.26 C189000500111 3.24 10.98 2.34 C189000500112 3.26 18.17 3.03 C189000500113 3.28 14.80 2.75 C189000500114 3.30 10.32 2.31 C189000500115 3.32 11.47 2.45 C189000500116 3.34 6.85 1.90 C189000500117 3.36 13.31 2.66 C189000500118 3.38 16.14 2.95 C189000500119 3.40 10.88 2.43 C189000500120 3.42 17.03 3.06 C189000500121 3.44 11.10 2.48 C189000500122 3.46 14.58 2.86 C189000500123 3.48 9.63 2.34 C189000500124 3.50 22.90 3.62 C189000500125 3.52 9.25 2.31 C189000500126 3.54 7.59 2.11 C189000500127 3.56 12.39 2.70 C189000500128 3.58 14.89 2.98 C189000500129 3.60 7.82 2.17 C189000500130 3.62 10.94 2.58 C189000500131 3.64 14.11 2.94 C189000500132 3.66 11.15 2.63 C189000500133 3.68 8.75 2.34 C189000500134 3.70 15.15 3.09 C189000500135 3.72 12.11 2.78 C189000500136 3.74 8.36 2.32 C189000500137 3.76 11.69 2.76 C189000500138 3.78 11.14 2.70 C189000500139 3.80 10.59 2.65 C189000500140 3.82 10.69 2.67 C189000500141 3.84 10.11 2.61 C189000500142 3.86 7.48 2.26 C189000500143 3.88 12.36 2.91 C189000500144 3.90 8.31 2.40 C189000500145 3.92 11.18 2.80 C189000500146 3.94 7.05 2.23 C189000500147 3.96 13.52 3.10 C189000500148 3.98 11.49 2.87 C189000500149 4.00 15.21 3.32 C189000500150 4.02 16.07 3.43 C189000500151 4.04 13.27 3.13 C189000500152 4.06 16.36 3.49 C189000500153 4.08 30.00 4.74 C189000500154 4.10 16.64 3.55 C189000500155 4.12 28.99 4.70 C189000500156 4.14 37.71 5.39 C189000500157 4.16 43.47 5.81 C189000500158 4.18 32.88 5.07 C189000500159 4.20 48.15 6.17 C189000500160 4.22 63.69 7.12 C189000500161 4.24 80.28 8.03 C189000500162 4.26 71.24 7.59 C189000500163 4.28 65.30 7.30 C189000500164 4.30 67.49 7.45 C189000500165 4.32 62.24 7.19 C189000500166 4.34 72.79 7.80 C189000500167 4.36 90.26 8.73 C189000500168 4.38 72.29 7.84 C189000500169 4.40 90.03 8.79 C189000500170 4.42 90.76 8.86 C189000500171 4.44 80.16 8.36 C189000500172 4.46 82.56 8.52 C189000500173 4.48 96.51 9.24 C189000500174 4.50 82.11 8.56 C189000500175 4.52 113.35 10.10 C189000500176 4.54 92.49 9.16 C189000500177 4.56 84.99 8.81 C189000500178 4.58 90.27 9.12 C189000500179 4.60 76.12 8.41 C189000500180 4.62 78.59 8.57 C189000500181 4.64 104.66 9.93 C189000500182 4.66 88.37 9.16 C189000500183 4.68 98.63 9.72 C189000500184 4.70 98.43 9.75 C189000500185 4.72 115.72 10.61 C189000500186 4.74 104.85 10.14 C189000500187 4.76 146.13 12.01 C189000500188 4.78 100.49 10.00 C189000500189 4.80 128.32 11.34 C189000500190 4.82 119.19 10.97 C189000500191 4.84 125.18 11.29 C189000500192 4.86 105.61 10.41 C189000500193 4.88 123.97 11.32 C189000500194 4.90 93.67 9.87 C189000500195 4.92 101.71 10.33 C189000500196 4.94 78.17 9.09 C189000500197 4.96 81.94 9.34 C189000500198 4.98 98.63 10.28 C189000500199 5.00 77.76 9.16 C189000500200 5.02 75.07 9.04 C189000500201 5.04 90.96 9.98 C189000500202 5.06 70.65 8.83 C189000500203 5.08 72.28 8.97 C189000500204 5.10 86.25 9.83 C189000500205 5.12 81.23 9.57 C189000500206 5.14 62.50 8.43 C189000500207 5.16 46.93 7.33 C189000500208 5.18 47.27 7.38 C189000500209 5.20 66.19 8.77 C189000500210 5.22 61.98 8.51 C189000500211 5.24 55.36 8.08 C189000500212 5.26 45.08 7.31 C189000500213 5.28 51.37 7.83 C189000500214 5.30 48.13 7.61 C189000500215 5.32 42.41 7.17 C189000500216 5.34 52.47 8.00 C189000500217 5.36 47.93 7.67 C189000500218 5.38 45.79 7.53 C189000500219 5.40 39.88 7.05 C189000500220 5.42 45.18 7.53 C189000500221 5.44 42.97 7.37 C189000500222 5.46 35.63 6.73 C189000500223 5.48 32.04 6.41 C189000500224 5.50 47.74 7.85 C189000500225 5.52 55.87 8.52 C189000500226 5.54 40.56 7.28 C189000500227 5.56 54.01 8.44 C189000500228 5.58 46.43 7.85 C189000500229 5.60 49.42 8.12 C189000500230 5.62 56.48 8.71 C189000500231 5.64 46.04 7.89 C189000500232 5.66 51.80 8.40 C189000500233 5.68 57.65 8.90 C189000500234 5.70 41.46 7.57 C189000500235 5.72 47.30 8.11 C189000500236 5.74 36.42 7.14 C189000500237 5.76 59.23 9.14 C189000500238 5.78 55.37 8.87 C189000500239 5.80 65.75 9.69 C189000500240 5.82 41.73 7.75 C189000500241 5.84 42.01 7.80 C189000500242 5.86 52.51 8.75 C189000500243 5.88 46.99 8.31 C189000500244 5.90 53.21 8.87 C189000500245 5.92 52.08 8.80 C189000500246 5.94 46.44 8.34 C189000500247 5.96 64.84 9.89 C189000500248 5.98 44.02 8.17 C189000500249 6.00 50.43 8.78 C189000500250 6.02 50.76 8.84 C189000500251 6.04 37.16 7.59 C189000500252 6.06 29.62 6.79 C189000500253 6.08 40.80 8.00 C189000500254 6.10 34.75 7.41 C189000500255 6.12 30.21 6.93 C189000500256 6.14 48.01 8.77 C189000500257 6.16 45.10 8.52 C189000500258 6.18 27.56 6.69 C189000500259 6.20 47.33 8.79 C189000500260 6.22 41.07 8.21 C189000500261 6.24 42.99 8.43 C189000500262 6.26 69.90 10.79 C189000500263 6.28 61.98 10.19 C189000500264 6.30 62.39 10.26 C189000500265 6.32 67.89 10.73 C189000500266 6.34 61.50 10.25 C189000500267 6.36 67.06 10.74 C189000500268 6.38 64.03 10.53 C189000500269 6.40 71.41 11.15 C189000500270 6.42 77.14 11.63 C189000500271 6.44 98.81 13.20 C189000500272 6.46 76.36 11.65 C189000500273 6.48 87.58 12.51 C189000500274 6.50 68.36 11.09 C189000500275 6.52 83.28 12.28 C189000500276 6.54 65.60 10.93 C189000500277 6.56 78.86 12.03 C189000500278 6.58 81.21 12.24 C189000500279 6.60 50.16 9.65 C189000500280 6.62 44.87 9.16 C189000500281 6.64 37.63 8.41 C189000500282 6.66 26.51 7.09 C189000500283 6.68 20.96 6.32 C189000500284 6.70 5.75 3.32 C189000500285 6.72 3.86 2.73 C189000500286 6.78 3.94 2.78 C189000500287 6.80 1.98 1.98 C189000500288 ENDDATA 266 0 C189000500289 ENDSUBENT 288 0 C189000599999 SUBENT C1890006 20120517 C118C189000600001 BIB 3 13 C189000600002 REACTION 1(2-HE-4(4-BE-7,0),,EN) C189000600003 2(2-HE-4(4-BE-7,0),,J) C189000600004 3(2-HE-4(4-BE-7,0),,PTY) C189000600005 4(2-HE-4(4-BE-7,TOT),,WID) C189000600006 5(2-HE-4(4-BE-7,EL),,WID) C189000600007 6(2-HE-4(4-BE-7,P),,WID) C189000600008 STATUS (TABLE) Data taken from tab.1 of the reference C189000600009 (DEP,C1890002) Resonance parameters determined from C189000600010 cross sections determined in present work C189000600011 (DEP,C1890003) C189000600012 (DEP,C1890004) C189000600013 (DEP,C1890005) C189000600014 ANALYSIS Resonance parameters determined by R-matrix analysis C189000600015 ENDBIB 13 0 C189000600016 NOCOMMON 0 0 C189000600017 DATA 9 11 C189000600018 DATA-CM 1DATA 2DATA 3DATA-CM 4DATA-ERR 4DATA-CM 5C189000600019 DATA-ERR 5DATA-CM 6DATA-ERR 6 C189000600020 MEV NO-DIM NO-DIM KEV KEV KEV C189000600021 KEV KEV KEV C189000600022 1.10 2.5 1.00 1.0 1.0 1.0 C189000600023 1.0 C189000600024 1.63 2.5 1.00 108.0 43.0 12.0 C189000600025 7.0 96.0 42.0 C189000600026 2.09 1.5 -1.00 378.0 56.0 156.0 C189000600027 20.0 222.0 52.0 C189000600028 2.08 2.5 -1.00 271.0 60.0 54.0 C189000600029 41.0 217.0 44.0 C189000600030 2.59 3.5 1.00 145.0 13.0 28.0 C189000600031 5.0 117.0 27.0 C189000600032 3.03 4.5 1.00 55.0 22.0 13.0 C189000600033 10.0 42.0 19.0 C189000600034 2.96 3.5 -1.00 306.0 65.0 92.0 C189000600035 41.0 214.0 51.0 C189000600036 4.44 3.5 1.00 467.0 112.0 365.0 C189000600037 103.0 102.0 43.0 C189000600038 4.86 4.5 1.00 542.0 82.0 452.0 C189000600039 74.0 90.0 35.0 C189000600040 5.88 2.5 1.00 743.0 66.0 734.0 C189000600041 65.0 8.0 8.0 C189000600042 6.26 2.5 -1.00 662.0 585.0 330.0 C189000600043 540.0 332.0 234.0 C189000600044 ENDDATA 26 0 C189000600045 ENDSUBENT 44 0 C189000699999 ENDENTRY 6 0 C189099999999