ENTRY L0262 20200712 L044L0262 0 1 SUBENT L0262001 20200712 L044L0262 1 1 BIB 12 38 L0262 1 2 TITLE Electric and magnetic dipole strength in 54Fe L0262 1 3 AUTHOR (R.Schwengner,R.Massarczyk,R.Beyer,M.Bhike,B.A.Brown, L0262 1 4 Krishichayan,K.Sieja,W.Tornow,D.Bemmerer,M.Butterling, L0262 1 5 V.Derya,M.Dietz,F.Fiedler,U.Friman-Gayer,A.Frotscher, L0262 1 6 M.Grieger,A.Hartmann,A.R.Junghans,T.Kogler,F.Ludwig, L0262 1 7 B.Lutz,H.Pai,T.Szucs,M.P.Takacs,A.Wagner) L0262 1 8 INSTITUTE (2GERZFK,1USALAS,1USADKE,1USATNL,1USAMSU,2FR ULP, L0262 1 9 2GERTHD,2GERDRE,3INDSAH) L0262 1 10 (2FR FR) CNRS Strasbourg L0262 1 11 REFERENCE (J,PR/C,101,064303,2020) L0262 1 12 FACILITY (LINAC,2GERZFK) Experiment performed at gELBE L0262 1 13 facility at Rossendorf. Electron beam was produced L0262 1 14 using low emittance superconducting linac with energy L0262 1 15 variable between 5 and 40 MeV, average beam current L0262 1 16 1.6 mA and micropulse duration 1-5 ps. L0262 1 17 SAMPLE (26-FE-54,ENR=0.993) Enriched metallic sample with L0262 1 18 diameter of 20 mm and weight of 1.4984 g. At gELBE, L0262 1 19 the target was combined with 0.300 g of boron, L0262 1 20 enriched to 99.5% in 11B. L0262 1 21 DETECTOR (HPGE) Scattered photons were measured with four HPGe L0262 1 22 detectors with relative efficiency of 100%, surrounded L0262 1 23 by escape-suppression shields made of 3 cm thick BGO L0262 1 24 scintillator L0262 1 25 METHOD (TOF) Time of flight was used to determine prompt L0262 1 26 gamma ray cross sections L0262 1 27 MONITOR (5-B-11(G,INL)5-B-11,,SIG) L0262 1 28 The known integrated scattering cross sections of L0262 1 29 states in 11B were used to determine the photon flux L0262 1 30 CORRECTION The measured cross section was corrected for inelastic L0262 1 31 transitions and branching ratios. L0262 1 32 INC-SOURCE (BRST) Photon beam was produced by bremstrahlung L0262 1 33 using electron beams of 7.5 and 13.9 MeV kinetic L0262 1 34 energy on Nb target foil with thickness of 5 and 12.5 L0262 1 35 mu-m, respectively. The photon beam was collimated by L0262 1 36 a 260-cm- long pure-aluminum collimator with a L0262 1 37 conical borehole of 8 mm in diameter at the entrance L0262 1 38 and 24 mm in diameter at the exit. L0262 1 39 HISTORY (20200712C) Compiled by S.H. L0262 1 40 ENDBIB 38 0 L0262 1 41 NOCOMMON 0 0 L0262 1 42 ENDSUBENT 41 0 L0262 199999 SUBENT L0262002 20200712 L044L0262 2 1 BIB 3 3 L0262 2 2 REACTION (26-FE-54(G,EL),,ARE) L0262 2 3 ERR-ANALYS (DATA-ERR) Origin of uncertainties not described L0262 2 4 STATUS (TABLE) Data taken from tab. 1 of the reference L0262 2 5 ENDBIB 3 0 L0262 2 6 NOCOMMON 0 0 L0262 2 7 DATA 4 103 L0262 2 8 EN-RES EN-RES-ERR DATA DATA-ERR L0262 2 9 KEV KEV B*EV B*EV L0262 2 10 1408.5 0.2 18.3 2.0 L0262 2 11 2958.5 0.3 8.1 1.1 L0262 2 12 3165.9 0.4 6.3 0.9 L0262 2 13 4581.7 0.7 5.4 1.4 L0262 2 14 5085.0 0.6 4.1 1.0 L0262 2 15 5114.1 0.3 4.7 0.7 L0262 2 16 5431.8 0.7 1.9 0.3 L0262 2 17 6127.8 0.3 15.0 1.5 L0262 2 18 6522.7 0.3 10.1 1.3 L0262 2 19 6787.6 0.9 5.8 0.7 L0262 2 20 6841.3 0.6 6.5 1.7 L0262 2 21 6914.2 0.9 6.3 1.3 L0262 2 22 6928.8 0.3 19.4 2.3 L0262 2 23 6946.5 0.6 9.6 1.8 L0262 2 24 6975.1 0.4 15.5 2.6 L0262 2 25 7072.9 0.9 5.6 1.4 L0262 2 26 7085.4 0.7 6.4 1.5 L0262 2 27 7120.9 0.4 21.0 2.9 L0262 2 28 7138.5 0.9 7.4 1.7 L0262 2 29 7334.8 0.7 6.7 1.5 L0262 2 30 7348.5 0.6 8.6 1.6 L0262 2 31 7367.3 0.4 17.4 2.5 L0262 2 32 7396.0 2.0 5.6 2.7 L0262 2 33 7415.4 0.3 79. 8. L0262 2 34 7447.2 0.3 32. 4. L0262 2 35 7469.7 1.2 9. 3. L0262 2 36 7487.4 0.4 42. 5. L0262 2 37 7553.3 0.9 22. 7. L0262 2 38 7631.3 0.4 33. 4. L0262 2 39 7645.8 0.5 23. 2.8 L0262 2 40 7723.2 0.5 31. 3. L0262 2 41 7898.2 0.5 19.7 2.8 L0262 2 42 7916.5 0.9 9.8 2.0 L0262 2 43 7933.8 0.2 55. 5. L0262 2 44 8014.8 0.2 344. 3. L0262 2 45 8093.2 0.2 106. 10. L0262 2 46 8119.2 0.2 148. 13. L0262 2 47 8163.7 0.7 22. 8. L0262 2 48 8219.6 0.2 589. 51. L0262 2 49 8265.3 0.7 11.2 2.8 L0262 2 50 8338.4 0.4 61. 6. L0262 2 51 8353.7 0.6 35. 4. L0262 2 52 8403.1 0.5 22. 3. L0262 2 53 8450.2 0.5 23. 3. L0262 2 54 8618.0 0.7 30. 4. L0262 2 55 8777.4 0.7 18. 5. L0262 2 56 8841.0 0.5 18.8 2.6 L0262 2 57 8855.5 0.2 102. 9. L0262 2 58 8897.1 0.3 67. 6. L0262 2 59 8930.3 0.7 17. 3. L0262 2 60 8986.0 0.2 142. 13. L0262 2 61 9065.2 0.3 130. 12. L0262 2 62 9113.1 0.2 94. 8. L0262 2 63 9128.9 0.7 13.8 2.3 L0262 2 64 9149.3 0.2 104. 9. L0262 2 65 9307.3 0.3 79. 8. L0262 2 66 9342.2 0.4 30. 4. L0262 2 67 9410.4 0.2 178. 16. L0262 2 68 9472.4 1.0 48. 18. L0262 2 69 9515.4 0.5 49. 7. L0262 2 70 9538.0 0.6 47. 7. L0262 2 71 9908.6 0.6 38. 7. L0262 2 72 9925.3 0.6 38. 5. L0262 2 73 10035.5 0.3 93. 9. L0262 2 74 10060.5 0.2 224. 20. L0262 2 75 10101.4 0.4 52. 6. L0262 2 76 10119.2 0.5 33. 4. L0262 2 77 10140.9 0.2 128. 12. L0262 2 78 10185.9 0.3 116. 14. L0262 2 79 10195.7 1.1 33. 9. L0262 2 80 10224.2 1.1 15. 4. L0262 2 81 10240.4 0.5 58. 7. L0262 2 82 10250.5 0.6 42. 6. L0262 2 83 10339.4 0.2 138. 13. L0262 2 84 10376.9 0.9 32. 9. L0262 2 85 10487.5 0.8 21. 8. L0262 2 86 10510.5 0.4 71. 11. L0262 2 87 10538.1 0.2 327. 29. L0262 2 88 10590.7 0.7 21. 6. L0262 2 89 10701.2 0.4 46. 5. L0262 2 90 10802.5 1.4 26. 9. L0262 2 91 10820.4 1.0 27. 8. L0262 2 92 10880.2 0.7 29. 4. L0262 2 93 10891.3 0.7 27. 4. L0262 2 94 10926.1 0.7 15. 3. L0262 2 95 11021.7 0.6 105. 17. L0262 2 96 11094.8 0.6 32. 5. L0262 2 97 11159.8 1.0 15. 3. L0262 2 98 11194.0 0.3 99. 9. L0262 2 99 11210.6 0.5 36. 4. L0262 2 100 11314.0 0.6 46. 6. L0262 2 101 11333.5 0.4 74. 8. L0262 2 102 11447.4 0.4 11.2 2.2 L0262 2 103 11480.6 0.6 37. 6. L0262 2 104 11530.6 0.3 156. 15. L0262 2 105 11561.4 1.2 17. 4. L0262 2 106 11761.1 1.4 6.8 1.9 L0262 2 107 11790.5 0.5 28. 4. L0262 2 108 11821.7 1.0 9.9 2.3 L0262 2 109 12273.2 0.5 27. 3. L0262 2 110 12397.0 0.7 25. 4. L0262 2 111 12902.5 0.8 29. 5. L0262 2 112 13171.4 1.5 6.0 1.0 L0262 2 113 ENDDATA 105 0 L0262 2 114 ENDSUBENT 113 0 L0262 299999 SUBENT L0262003 20200712 L044L0262 3 1 BIB 3 11 L0262 3 2 REACTION (26-FE-54(G,SCT)26-FE-54,,SIG) L0262 3 3 ERR-ANALYS (ERR-T) Total uncertainty consisting of L0262 3 4 -statistical uncertainty of the spectrum L0262 3 5 -systematic uncertainty in detector efficiency L0262 3 6 -systematic uncertainty in photon flux based on L0262 3 7 uncertainties of monitor cross section. L0262 3 8 (ERR-1) Systematic uncertainty in detector efficiency L0262 3 9 (DATA-ERR) Systematic uncertainty of strength-function L0262 3 10 and level-density models, not included in ERR-TL0262 3 11 STATUS (TABLE) Data taken from tab. 2 of the reference L0262 3 12 (COREL,L0262004) Data measured with E0=13.9 MeV L0262 3 13 ENDBIB 11 0 L0262 3 14 COMMON 2 3 L0262 3 15 ERR-1 DATA-ERR L0262 3 16 PER-CENT PER-CENT L0262 3 17 5. 20. L0262 3 18 ENDCOMMON 3 0 L0262 3 19 DATA 3 30 L0262 3 20 EN DATA ERR-T L0262 3 21 KEV MB MB L0262 3 22 4.3 0.16 0.04 L0262 3 23 4.4 0.24 0.08 L0262 3 24 4.5 0.017 0.009 L0262 3 25 4.6 0.31 0.15 L0262 3 26 4.9 0.50 0.05 L0262 3 27 5.0 0.33 0.10 L0262 3 28 5.1 0.49 0.08 L0262 3 29 5.2 0.18 0.05 L0262 3 30 5.3 0.15 0.03 L0262 3 31 5.4 0.21 0.05 L0262 3 32 5.5 0.18 0.08 L0262 3 33 5.7 0.26 0.04 L0262 3 34 5.8 0.12 0.06 L0262 3 35 5.9 0.12 0.05 L0262 3 36 6.0 0.41 0.18 L0262 3 37 6.1 0.70 0.27 L0262 3 38 6.2 0.25 0.03 L0262 3 39 6.3 0.53 0.07 L0262 3 40 6.4 0.45 0.08 L0262 3 41 6.5 1.04 0.10 L0262 3 42 6.6 0.45 0.04 L0262 3 43 6.7 0.60 0.05 L0262 3 44 6.8 0.82 0.05 L0262 3 45 6.9 0.63 0.08 L0262 3 46 7.0 0.44 0.05 L0262 3 47 7.1 0.72 0.05 L0262 3 48 7.2 0.49 0.04 L0262 3 49 7.3 0.75 0.05 L0262 3 50 7.4 1.58 0.08 L0262 3 51 7.5 1.19 0.07 L0262 3 52 ENDDATA 32 0 L0262 3 53 ENDSUBENT 52 0 L0262 399999 SUBENT L0262004 20200712 L044L0262 4 1 BIB 3 11 L0262 4 2 REACTION (26-FE-54(G,SCT)26-FE-54,,SIG) L0262 4 3 ERR-ANALYS (ERR-T) Total uncertainty consisting of L0262 4 4 -statistical uncertainty of the spectrum L0262 4 5 -systematic uncertainty in detector efficiency, L0262 4 6 -systematic uncertainty in photon flux based on L0262 4 7 uncertainties of monitor cross section. L0262 4 8 (ERR-1) Systematic uncertainty in detector efficiency L0262 4 9 (DATA-ERR) Systematic uncertainty of strength-function L0262 4 10 and level-density models, not included in ERR-TL0262 4 11 STATUS (TABLE) Data taken from tab. 3 of the reference L0262 4 12 (COREL,L0262003) Data measured with E0=7.5 MeV L0262 4 13 ENDBIB 11 0 L0262 4 14 COMMON 2 3 L0262 4 15 ERR-1 DATA-ERR L0262 4 16 PER-CENT PER-CENT L0262 4 17 5. 20. L0262 4 18 ENDCOMMON 3 0 L0262 4 19 DATA 3 61 L0262 4 20 EN DATA ERR-T L0262 4 21 KEV MB MB L0262 4 22 7.0 1.1 0.8 L0262 4 23 7.2 3.3 3.1 L0262 4 24 7.3 1.6 0.8 L0262 4 25 7.4 1.2 0.8 L0262 4 26 7.5 2.1 1.3 L0262 4 27 7.7 2.6 1.9 L0262 4 28 7.8 3.6 1.4 L0262 4 29 8.1 5.8 4.1 L0262 4 30 8.2 12.2 2.2 L0262 4 31 8.3 2.9 0.8 L0262 4 32 8.4 3.3 0.7 L0262 4 33 8.5 3.7 0.8 L0262 4 34 8.6 6.7 1.7 L0262 4 35 8.7 3.6 0.9 L0262 4 36 8.8 3.6 1.1 L0262 4 37 8.9 4.2 1.3 L0262 4 38 9.0 14.8 3.4 L0262 4 39 9.1 8.1 1.6 L0262 4 40 9.2 7.8 0.13 L0262 4 41 9.3 4.6 0.8 L0262 4 42 9.4 11.0 2.5 L0262 4 43 9.5 4.1 1.3 L0262 4 44 9.6 6.7 1.0 L0262 4 45 9.7 4.5 1.3 L0262 4 46 9.8 5.9 0.8 L0262 4 47 9.9 8.4 1.0 L0262 4 48 10.0 10.9 0.9 L0262 4 49 10.1 17.5 1.4 L0262 4 50 10.2 14.4 1.1 L0262 4 51 10.3 11.6 0.9 L0262 4 52 10.4 8.9 0.7 L0262 4 53 10.5 18.0 1.3 L0262 4 54 10.6 6.6 0.6 L0262 4 55 10.7 7.6 0.6 L0262 4 56 10.8 7.9 0.6 L0262 4 57 10.9 9.5 0.9 L0262 4 58 11.0 10.2 0.8 L0262 4 59 11.1 10.7 0.8 L0262 4 60 11.2 12.4 0.7 L0262 4 61 11.3 12.6 0.6 L0262 4 62 11.4 7.6 0.5 L0262 4 63 11.5 14.0 1.1 L0262 4 64 11.6 8.5 0.7 L0262 4 65 11.7 6.8 0.7 L0262 4 66 11.8 9.4 0.9 L0262 4 67 11.9 9.5 0.9 L0262 4 68 12.0 8.4 0.9 L0262 4 69 12.1 7.7 0.9 L0262 4 70 12.2 7.3 0.8 L0262 4 71 12.3 9.7 1.1 L0262 4 72 12.4 8.9 1.0 L0262 4 73 12.5 7.4 1.0 L0262 4 74 12.6 8.0 1.0 L0262 4 75 12.7 9.3 1.2 L0262 4 76 12.8 6.1 0.9 L0262 4 77 12.9 10.7 1.3 L0262 4 78 13.0 7.3 1.1 L0262 4 79 13.1 5.4 0.9 L0262 4 80 13.2 9.8 1.3 L0262 4 81 13.3 6.2 1.1 L0262 4 82 13.4 5.5 0.9 L0262 4 83 ENDDATA 63 0 L0262 4 84 ENDSUBENT 83 0 L0262 499999 ENDENTRY 4 0 L026299999999