ENTRY O1297 20221225 O092O1297 0 1 SUBENT O1297001 20221225 O092O1297 1 1 BIB 12 51 O1297 1 2 TITLE Production cross-sections from neutron-deficient 92-Mo O1297 1 3 at 500*A MeV O1297 1 4 REFERENCE (J,EPJ/A,25,(2),193,2005) O1297 1 5 (J,EPJ/A,25,(3),473,2005) ERRATUM. O1297 1 6 (J,JP/G,31,S1843,2005) - same data at figs. O1297 1 7 AUTHOR (B.Fernandez-Dominguez, R.C.Lemmon, B.Blank, O1297 1 8 M.Chartier, D.Cortina-Gil, J.L.Durell, H.Geissel, O1297 1 9 J.Gerl, S.Mandal, F.Rejmund, K.Suemmerer) O1297 1 10 INSTITUTE (2UK LVP,2UK DAR,2FR GRA,2SPNSAU,2UK MAN,2GERGSI, O1297 1 11 2FR GAN) O1297 1 12 FACILITY (SYNCH,2GERGSI) O1297 1 13 SAMPLE The 92-Mo ions were directed onto a beryllium target O1297 1 14 of thickness 4007.0 mg/cm2 placed at the entrance of O1297 1 15 the fragment separator. O1297 1 16 DETECTOR (SCIN) Two plastic scintillators mounted at the O1297 1 17 dispersive and achromatic focal planes. O1297 1 18 (IOCH) O1297 1 19 (MWPC) Two multiwire chambers. O1297 1 20 METHOD (EXTB) The average intensity was 109 particles/spill. O1297 1 21 (SITA) O1297 1 22 (BCINT) The number of incident ions was recorded by theO1297 1 23 secondary-electron monitor SEETRAM placed before the O1297 1 24 production target. O1297 1 25 (EDE,TOF) O1297 1 26 Inverse geometry. O1297 1 27 COMMENT -By authors. The ions of interest were identified by O1297 1 28 combining measurements of their magnetic rigidity, O1297 1 29 energy loss, and time of flight. The plastic O1297 1 30 scintillators mounted at the dispersive intermediate O1297 1 31 and achromatic focal planes, were used to determine O1297 1 32 the horizontal positions of the fragments and their O1297 1 33 time of flight. At the final focal plane two O1297 1 34 multiwire chambers provided the position measurement O1297 1 35 for the calibrations. Finally, from the energy loss O1297 1 36 measurement in the ionisation chamber the nuclear O1297 1 37 charge was obtained, since all the produced fragments O1297 1 38 were fully stripped. O1297 1 39 ERR-ANALYS (ERR-T) Total uncertainty of production cross section. O1297 1 40 Mean systematical uncertainties contributing to the O1297 1 41 determination of the production cross-sections. O1297 1 42 (ERR-1) Uncertainty in target thickness = 0.1%. O1297 1 43 (ERR-2) Uncertainty in SEETRAM calibration = 1%. O1297 1 44 (ERR-3,2.,54.) Uncertainty in SEETRAM offset = 2-54% O1297 1 45 (ERR-4,10.,75.) Uncertainty in transmission = 10-75% O1297 1 46 (ERR-S,1.,33.) Statistical uncertainty in = 1-33% O1297 1 47 STATUS (TABLE) Tbl. 2 from Europ.Phys.J.,A25(2005)193 O1297 1 48 HISTORY (20051011C) O1297 1 49 (20060210U) Last checking has been done. O1297 1 50 (20220202U) SD: Ref. EPJ/A,25,193 -> EPJ/A,25,(2),193 O1297 1 51 ERR-ANALYS updated. O1297 1 52 (20221225A) SD: Ref. added. Correction in Subent 002. O1297 1 53 ENDBIB 51 0 O1297 1 54 COMMON 3 3 O1297 1 55 EN ERR-1 ERR-2 O1297 1 56 GEV PER-CENT PER-CENT O1297 1 57 46. 0.1 1. O1297 1 58 ENDCOMMON 3 0 O1297 1 59 ENDSUBENT 58 0 O1297 199999 SUBENT O1297002 20221225 O092O1297 2 1 BIB 3 3 O1297 2 2 REACTION (4-BE-9(42-MO-92,X)ELEM/MASS,,SIG) O1297 2 3 FLAG (1.) Zero uncertainty is shown in data table. O1297 2 4 HISTORY (20221225A) SD: SF5=IND deleted from REACTION code. O1297 2 5 ENDBIB 3 0 O1297 2 6 NOCOMMON 0 0 O1297 2 7 DATA 5 89 O1297 2 8 ELEMENT MASS DATA ERR-T FLAG O1297 2 9 NO-DIM NO-DIM MB MB NO-DIM O1297 2 10 31. 72. 0.094 0.03 O1297 2 11 31. 73. 0.027 0.005 O1297 2 12 32. 73. 0.27 0.11 O1297 2 13 32. 74. 0.15 0.03 O1297 2 14 32. 75. 0.051 0.008 O1297 2 15 32. 76. 0.012 0.003 O1297 2 16 33. 75. 0.43 0.21 O1297 2 17 33. 76. 0.18 0.04 O1297 2 18 33. 77. 0.053 0.008 O1297 2 19 33. 78. 0.022 0.004 O1297 2 20 34. 76. 0.92 0.38 O1297 2 21 34. 77. 1.2 0.1 O1297 2 22 34. 78. 0.39 0.05 O1297 2 23 34. 79. 0.089 0.016 O1297 2 24 34. 80. 0.029 0.004 O1297 2 25 35. 78. 5.2 1.3 O1297 2 26 35. 79. 2.2 0.3 O1297 2 27 35. 80. 0.7 0.08 O1297 2 28 35. 81. 0.17 0.02 O1297 2 29 35. 82. 0.042 0.005 O1297 2 30 36. 79. 7.7 0.6 O1297 2 31 36. 80. 12. 1. O1297 2 32 36. 81. 5.1 0.4 O1297 2 33 36. 82. 1.4 0.1 O1297 2 34 36. 83. 0.24 0.03 O1297 2 35 36. 84. 0.047 0.009 O1297 2 36 37. 75. 0.12 0.07 O1297 2 37 37. 77. 7.8 3.5 O1297 2 38 37. 78. 14. 10. O1297 2 39 37. 79. 30. 16. O1297 2 40 37. 80. 49. 21. O1297 2 41 37. 81. 44. 18. O1297 2 42 37. 82. 15. 1. O1297 2 43 37. 83. 8.7 0.5 O1297 2 44 37. 84. 2.4 0.2 O1297 2 45 37. 85. 0.44 0.04 O1297 2 46 37. 86. 0.057 0.013 O1297 2 47 38. 75. 0.00012 0.00004 O1297 2 48 38. 76. 0.00051 0.00019 O1297 2 49 38. 77. 0.0078 0.0019 O1297 2 50 38. 78. 0.2 0.08 O1297 2 51 38. 79. 1.9 0.8 O1297 2 52 38. 80. 3.5 1.5 O1297 2 53 38. 81. 21. 7. O1297 2 54 38. 82. 61. 25. O1297 2 55 38. 83. 118. 45. O1297 2 56 38. 84. 40. 10. O1297 2 57 38. 85. 12. 1. O1297 2 58 38. 86. 4.9 0.4 O1297 2 59 38. 87. 0.72 0.04 O1297 2 60 38. 88. 0.092 0.02 O1297 2 61 39. 78. 0.00017 0.00001 O1297 2 62 39. 79. 0.019 0.006 O1297 2 63 39. 80. 0.004 0.0008 O1297 2 64 39. 81. 1.3 0.4 O1297 2 65 39. 82. 6.8 3.9 O1297 2 66 39. 83. 18. 6. O1297 2 67 39. 84. 45. 17. O1297 2 68 39. 85. 104. 42. O1297 2 69 39. 87. 25. 1. O1297 2 70 39. 88. 5.9 0.2 O1297 2 71 39. 89. 1.4 0.1 O1297 2 72 40. 79. 0.4 1. O1297 2 73 40. 80. 0.00011 1. O1297 2 74 40. 81. 0.0039 0.0009 O1297 2 75 40. 82. 0.052 0.008 O1297 2 76 40. 83. 0.52 0.15 O1297 2 77 40. 84. 4.8 2.5 O1297 2 78 40. 85. 19. 1. O1297 2 79 40. 86. 38. 13. O1297 2 80 40. 87. 69. 26. O1297 2 81 40. 90. 25. 2. O1297 2 82 40. 91. 0.44 0.1 O1297 2 83 41. 82. 0.000039 0.000005 O1297 2 84 41. 83. 0.0062 0.0044 O1297 2 85 41. 84. 0.031 0.006 O1297 2 86 41. 85. 0.086 0.023 O1297 2 87 41. 86. 1.4 0.5 O1297 2 88 41. 87. 4. 2. O1297 2 89 41. 88. 33. 13. O1297 2 90 41. 89. 33. 11. O1297 2 91 42. 84. 0.000028 0.000005 O1297 2 92 42. 85. 0.00033 0.0002 O1297 2 93 42. 86. 0.015 0.004 O1297 2 94 42. 87. 0.04 0.01 O1297 2 95 42. 88. 4.1 2.4 O1297 2 96 42. 89. 2.6 1.3 O1297 2 97 42. 90. 147. 111. O1297 2 98 42. 91. 49. 19. O1297 2 99 ENDDATA 91 0 O1297 2 100 ENDSUBENT 99 0 O1297 299999 ENDENTRY 2 0 O129799999999