ENTRY E1640 20120523 E068E164000000001 SUBENT E1640001 20120523 E068E164000100001 BIB 11 38 E164000100002 TITLE Anomaly in the 15N, 16O, 19F + 54,56Fe fusion cross E164000100003 sections around the Coulomb barrier energy E164000100004 AUTHOR (H.Funaki, E.Arai) E164000100005 INSTITUTE (2JPNTIT) E164000100006 REFERENCE (J,NP/A,556,(2),307,199305) E164000100007 SAMPLE - Chemical-form of target: Fe2O3 E164000100008 - Physical-form of target is solid. E164000100009 - Backing is carbon. E164000100010 - Backing-thickness is 0.020 mg/cm**2. E164000100011 METHOD (TOF) E164000100012 FACILITY (LINAC,2JPNTIT) Heavy Ion Linac System E164000100013 DETECTOR - Detector resolution: The mass separation of the E164000100014 spectrometer has been mainly determined by the E164000100015 energy resolution to be delta A = 4 in the A-region E164000100016 around 70. E164000100017 - Calibration: The beam energy analyzing magnet has E164000100018 been calibrated by measuring the sharp peak observed E164000100019 at 6.42 MeV in the 1H(19F,alpha gamma)16O reaction. E164000100020 (TELES) The t.o.f. counter telescope has two timing E164000100021 detectors which define a flight path of 50 cm. E164000100022 (SIBAR) A 100 mm**2 surface-barrier detector (SBD) E164000100023 provides the kinetic energy (E) signal of E164000100024 particles. E164000100025 ADD-RES E1640.002:26-FE-54(9-F-19,FUS) E164000100026 Angular distribution (Angular distribution E164000100027 of evaporation residues) E164000100028 See NRDF D1640 DATA,1 for detail. E164000100029 E1640.003:26-FE-54(9-F-19,FUS) E164000100030 Angular distribution (Angular distribution E164000100031 of evaporation residues) E164000100032 See NRDF D1640 DATA,2 for detail. E164000100033 REL-REF (N,,E.Arai+,J,NIM/B,64,296,1992) E164000100034 Detailed description of the system is given E164000100035 HISTORY (20030912T) Km + Am + On. Data converted from NRDF E164000100036 D1640 E164000100037 (20070510U) On. MeV/u -> MeV/A in free text fields E164000100038 (20111020A) Nf. PART-DET deleted, 004-009 REACTION E164000100039 corrected E164000100040 ENDBIB 38 0 E164000100041 NOCOMMON 0 0 E164000100042 ENDSUBENT 41 0 E164000199999 NOSUBENT E1640002 20040311 0000E164000200001 NOSUBENT E1640003 20040311 0000E164000300001 SUBENT E1640004 20120523 E068E164000400001 BIB 8 16 E164000400002 REACTION (26-FE-54(7-N-15,FUS),,SIG,ER) E164000400003 INC-SPECT EN: The final energy of beams has been raised or E164000400004 lowered by the second linac in the range between 2 and E164000400005 3 MeV/u. E164000400006 SAMPLE Target-thickness is 0.110 mg/cm**2. The thickness was E164000400007 determined by the Rutherford backscattering technique. E164000400008 (26-FE-54,ENR=0.9721) E164000400009 ANALYSIS (INTAD) Integration of differential cross sections E164000400010 (angular distributions of evaporation residue) E164000400011 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000400012 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000400013 barrier-penetration model [C.H.Dasso et al. E164000400014 Comput.Phys.Commun.46(1987)187]) E164000400015 STATUS (CURVE) Scanned from Fig.3 (a), p310 in reference E164000400016 HISTORY (20061122A) Mh. Re-digitized E164000400017 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000400018 ENDBIB 16 0 E164000400019 NOCOMMON 0 0 E164000400020 DATA 3 10 E164000400021 EN-CM DATA DATA-ERR E164000400022 MEV MB MB E164000400023 2.482E+01 2.818E+01 6.670E+00 E164000400024 2.601E+01 8.445E+01 1.176E+01 E164000400025 2.661E+01 1.078E+02 6.528E+00 E164000400026 2.751E+01 1.801E+02 E164000400027 2.771E+01 1.870E+02 E164000400028 2.841E+01 3.074E+02 3.444E+01 E164000400029 2.954E+01 2.973E+02 5.003E+01 E164000400030 3.270E+01 6.508E+02 7.294E+01 E164000400031 3.436E+01 7.739E+02 7.339E+01 E164000400032 3.568E+01 6.504E+02 4.128E+01 E164000400033 ENDDATA 12 0 E164000400034 ENDSUBENT 33 0 E164000499999 SUBENT E1640005 20120523 E068E164000500001 BIB 8 16 E164000500002 REACTION (26-FE-56(7-N-15,FUS),,SIG,ER) E164000500003 INC-SPECT EN: The final energy of beams has been raised or E164000500004 lowered by the second linac in the range between 2 and E164000500005 3 MeV/A. E164000500006 SAMPLE Target-thickness is 0.080 mg/cm**2. The thickness was E164000500007 determined by the Rutherford backscattering technique. E164000500008 (26-FE-56,ENR=0.9993) E164000500009 ANALYSIS (INTAD) Integration of differential cross sections E164000500010 (angular distributions of evaporation residue) E164000500011 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000500012 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000500013 barrier-penetration model [C.H.Dasso et al. E164000500014 Comput.Phys.Commun.46(1987)187]) E164000500015 STATUS (CURVE) Scanned from Fig.3 (b), p310 in reference E164000500016 HISTORY (20061122A) Mh. Re-digitized E164000500017 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000500018 ENDBIB 16 0 E164000500019 NOCOMMON 0 0 E164000500020 DATA 3 10 E164000500021 EN-CM DATA DATA-ERR E164000500022 MEV MB MB E164000500023 2.499E+01 4.911E+01 1.365E+01 E164000500024 2.623E+01 9.096E+01 1.471E+01 E164000500025 2.694E+01 9.992E+01 9.229E+00 E164000500026 2.774E+01 1.721E+02 1.465E+01 E164000500027 2.802E+01 1.914E+02 1.629E+01 E164000500028 2.863E+01 2.807E+02 3.402E+01 E164000500029 2.972E+01 3.647E+02 4.964E+01 E164000500030 3.286E+01 7.345E+02 8.736E+01 E164000500031 3.456E+01 8.457E+02 8.782E+01 E164000500032 3.599E+01 8.292E+02 5.554E+01 E164000500033 ENDDATA 12 0 E164000500034 ENDSUBENT 33 0 E164000599999 SUBENT E1640006 20120523 E068E164000600001 BIB 9 18 E164000600002 REACTION (26-FE-54(8-O-16,FUS),,SIG,ER) E164000600003 INC-SOURCE - Beam intensity is 10 nA. E164000600004 - Charge of incident ion is 7+. E164000600005 INC-SPECT EN: The final energy of beams has been raised or E164000600006 lowered by the second linac in the range between 2 and E164000600007 3 MeV/A. E164000600008 SAMPLE Target-thickness is 0.110 mg/cm**2. The thickness was E164000600009 determined by the Rutherford backscattering technique. E164000600010 (26-FE-54,ENR=0.9721) E164000600011 ANALYSIS (INTAD) Integration of differential cross sections E164000600012 (angular distributions of evaporation residue) E164000600013 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000600014 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000600015 barrier-penetration model [C.H.Dasso et al. E164000600016 Comput.Phys.Commun.46(1987)187]) E164000600017 STATUS (CURVE) Scanned from Fig.3 (c), p310 in reference E164000600018 HISTORY (20061122A) Mh. Re-digitized E164000600019 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000600020 ENDBIB 18 0 E164000600021 NOCOMMON 0 0 E164000600022 DATA 3 6 E164000600023 EN-CM DATA DATA-ERR E164000600024 MEV MB MB E164000600025 2.808E+01 6.660E+00 1.387E+00 E164000600026 2.970E+01 2.883E+01 3.116E+00 E164000600027 3.211E+01 1.480E+02 E164000600028 3.472E+01 3.249E+02 E164000600029 3.720E+01 4.161E+02 2.772E+01 E164000600030 3.962E+01 5.603E+02 E164000600031 ENDDATA 8 0 E164000600032 ENDSUBENT 31 0 E164000699999 SUBENT E1640007 20120523 E068E164000700001 BIB 9 18 E164000700002 REACTION (26-FE-56(8-O-16,FUS),,SIG,ER) E164000700003 INC-SOURCE - Beam intensity is 10 nA. E164000700004 - Charge of incident ion is 7+. E164000700005 INC-SPECT EN: The final energy of beams has been raised or E164000700006 lowered by the second linac in the range between 2 and E164000700007 3 MeV/A. E164000700008 SAMPLE Target-thickness is 0.080 mg/cm**2. The thickness was E164000700009 determined by the Rutherford backscattering technique. E164000700010 (26-FE-56,ENR=0.9993) E164000700011 ANALYSIS (INTAD) Integration of differential cross sections E164000700012 (angular distributions of evaporation residue) E164000700013 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000700014 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000700015 barrier-penetration model [C.H.Dasso et al. E164000700016 Comput.Phys.Commun.46(1987)187]) E164000700017 STATUS (CURVE) Scanned from Fig.3 (d), p310 in reference E164000700018 HISTORY (20061122A) Mh. Re-digitized E164000700019 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000700020 ENDBIB 18 0 E164000700021 NOCOMMON 0 0 E164000700022 DATA 3 6 E164000700023 EN-CM DATA DATA-ERR E164000700024 MEV MB MB E164000700025 2.842E+01 2.002E+01 5.451E+00 E164000700026 2.992E+01 6.040E+01 1.060E+01 E164000700027 3.241E+01 1.768E+02 1.839E+01 E164000700028 3.501E+01 3.987E+02 3.427E+01 E164000700029 3.752E+01 4.790E+02 4.289E+01 E164000700030 3.989E+01 6.544E+02 6.095E+01 E164000700031 ENDDATA 8 0 E164000700032 ENDSUBENT 31 0 E164000799999 SUBENT E1640008 20120523 E068E164000800001 BIB 8 16 E164000800002 REACTION (26-FE-54(9-F-19,FUS),,SIG,ER) E164000800003 INC-SPECT EN: The final energy of beams has been raised or E164000800004 lowered by the second linac in the range between 2 and E164000800005 3 MeV/A. E164000800006 SAMPLE Target-thickness is 0.110 mg/cm**2. The thickness was E164000800007 determined by the Rutherford backscattering technique. E164000800008 (26-FE-54,ENR=0.9721) E164000800009 ANALYSIS (INTAD) Integration of differential cross sections E164000800010 (angular distributions of evaporation residue) E164000800011 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000800012 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000800013 barrier-penetration model [C.H.Dasso et al. E164000800014 Comput.Phys.Commun.46(1987)187]) E164000800015 STATUS (CURVE) Scanned from Fig.3 (e), p310 in reference E164000800016 HISTORY (20061122A) Mh. Re-digitized E164000800017 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000800018 ENDBIB 16 0 E164000800019 NOCOMMON 0 0 E164000800020 DATA 3 10 E164000800021 EN-CM DATA DATA-ERR E164000800022 MEV MB MB E164000800023 3.091E+01 2.980E+01 5.143E+00 E164000800024 3.164E+01 3.776E+01 4.000E+00 E164000800025 3.229E+01 5.003E+01 5.793E+00 E164000800026 3.311E+01 6.727E+01 1.004E+01 E164000800027 3.392E+01 1.110E+02 9.592E+00 E164000800028 3.551E+01 1.777E+02 1.985E+01 E164000800029 3.711E+01 2.658E+02 4.150E+01 E164000800030 3.842E+01 3.348E+02 4.886E+01 E164000800031 4.006E+01 4.281E+02 5.241E+01 E164000800032 4.148E+01 5.330E+02 6.525E+01 E164000800033 ENDDATA 12 0 E164000800034 ENDSUBENT 33 0 E164000899999 SUBENT E1640009 20120523 E068E164000900001 BIB 8 16 E164000900002 REACTION (26-FE-56(9-F-19,FUS),,SIG,ER) E164000900003 INC-SPECT EN: The final energy of beams has been raised or E164000900004 lowered by the second linac in the range between 2 and E164000900005 3 MeV/A. E164000900006 SAMPLE Target-thickness is 0.080 mg/cm**2. The thickness was E164000900007 determined by the Rutherford backscattering technique. E164000900008 (26-FE-56,ENR=0.9993) E164000900009 ANALYSIS (INTAD) Integration of differential cross sections E164000900010 (angular distributions of evaporation residue) E164000900011 ERR-ANALYS (DATA-ERR) No information on source of uncertainties E164000900012 ADD-RES (COMP) Coupled channel method (the one-dimensional E164000900013 barrier-penetration model [C.H.Dasso et al. E164000900014 Comput.Phys.Commun.46(1987)187]) E164000900015 STATUS (CURVE) Scanned from Fig.3 (f), p310 in reference E164000900016 HISTORY (20061122A) Mh. Re-digitized E164000900017 (20111020A) Nf. REACTION corrected SIG -> SIG,ER E164000900018 ENDBIB 16 0 E164000900019 NOCOMMON 0 0 E164000900020 DATA 3 10 E164000900021 EN-CM DATA DATA-ERR E164000900022 MEV MB MB E164000900023 3.122E+01 3.509E+01 5.632E+00 E164000900024 3.192E+01 4.794E+01 6.017E+00 E164000900025 3.274E+01 6.569E+01 9.866E+00 E164000900026 3.347E+01 8.973E+01 1.139E+01 E164000900027 3.426E+01 1.575E+02 2.156E+01 E164000900028 3.588E+01 2.216E+02 2.096E+01 E164000900029 3.743E+01 2.983E+02 3.013E+01 E164000900030 3.884E+01 3.461E+02 3.496E+01 E164000900031 4.044E+01 4.270E+02 4.039E+01 E164000900032 4.195E+01 5.732E+02 4.876E+01 E164000900033 ENDDATA 12 0 E164000900034 ENDSUBENT 33 0 E164000999999 ENDENTRY 9 0 E164099999999