ENTRY O0924 20140305 O052O092400000001 SUBENT O0924001 20140305 O052O092400100001 BIB 14 36 O092400100002 TITLE Superasymmetric fission at intermediate energy and O092400100003 production of neutron-rich nuclei with A< 80. O092400100004 AUTHOR (M.Huhta, P.Dendooven, A.Honkanen, A.Jokinen, O092400100005 G.Lhersonneau, M.Oinonen, H.Penttila, K.Perajarvi, O092400100006 V.A.Rubchenya, J.Aysto) O092400100007 INSTITUTE (2SF JYV) O092400100008 (4RUSRI) O092400100009 REFERENCE (J,PL/B,405,230,1997) O092400100010 REL-REF (N,O0646001,E.Karttunen+,J,NSE,109,350,1991) O092400100011 (N,O0499001,P.P.Jauho+,J,PR/C,49,2036,1994) O092400100012 Theoretical models. O092400100013 (M,O0825001,M.Leino+,J,PR/C,44,336,1991) Details of O092400100014 experiment. O092400100015 SAMPLE The 15 mg/cm**2 thick uranium target foil were used. O092400100016 ADD-RES (COMP).The theoretical model for calculating mass and O092400100017 independent fission products. O092400100018 (G-SPC) O092400100019 PART-DET (DG) O092400100020 (B-) O092400100021 COMMENT -By authors. Independent and cumulative fission productO092400100022 yields in atoms/s for Z=28-32 and A=71-82 as measured O092400100023 at the focal point of the IGISOL separator. O092400100024 FACILITY (OLMS,2SF JYV) The on-line mass separator IGISOL. O092400100025 (CYCLO,2SF JYV) O092400100026 METHOD (OLMS) O092400100027 (HEJET) Fragments were slowed down as ions in O092400100028 high-pressure helium and transported by the flow into O092400100029 the mass separator. O092400100030 (ACTIV) O092400100031 (BCINT) O092400100032 ERR-ANALYS (DATA-ERR) Experimental error O092400100033 STATUS (TABLE) Data were received from Dr. V.A.Rubchenya O092400100034 HISTORY (20011228C) O092400100035 (20030503U) Last checking has been done. O092400100036 (20140305A) SD: Data from author presented in D0149 O092400100037 were added. ERR-T -> DATA-ERR in Subent 2,3. O092400100038 ENDBIB 36 0 O092400100039 COMMON 1 3 O092400100040 EN O092400100041 MEV O092400100042 25. O092400100043 ENDCOMMON 3 0 O092400100044 ENDSUBENT 43 0 O092400199999 SUBENT O0924002 20140305 O052O092400200001 BIB 5 13 O092400200002 REACTION (92-U-238(P,X)ELEM/MASS,IND,FY) O092400200003 The independent yields extracted from the measured O092400200004 cumulative production yields, which were determined O092400200005 from the radioactivity of the mass separated nuclides. O092400200006 MISC-COL (MISC) Independent fission product yield in atoms/s O092400200007 ERR-ANALYS (MISC-ERR) Experimental error O092400200008 COMMENT - By authors. The average masses, standard deviations O092400200009 and elemental yields were obtained by fitting with a O092400200010 gaussian function. O092400200011 HISTORY (20140305A) SD: SF8=REL deleted, SF6=PY -> FY in O092400200012 REACTION code values from col. DATA were moved O092400200013 MISC-COL; absolute values received from author were O092400200014 added in col.DATA from D0149.002 O092400200015 ENDBIB 13 0 O092400200016 NOCOMMON 0 0 O092400200017 DATA 6 21 O092400200018 ELEMENT MASS DATA DATA-ERR MISC MISC-ERR O092400200019 NO-DIM NO-DIM PRD/FIS PRD/FIS ARB-UNITS ARB-UNITS O092400200020 28. 71. 8.51E-5 2.54E-5 5.7 1.7 O092400200021 29. 71. 2.09E-5 1.64E-5 1.4 1.1 O092400200022 29. 72. 2.3E-4 4.03E-5 15. 3. O092400200023 29. 73. 1.46E-4 4.78E-5 10. 3. O092400200024 29. 74. 1.39E-4 4.48E-5 9. 3. O092400200025 30. 74. 2.43E-4 7.16E-5 16. 5. O092400200026 30. 75. 0.00103 1.13E-4 69. 8. O092400200027 30. 76. 8.25E-4 7.31E-5 55. 5. O092400200028 30. 77. 3.97E-4 5.67E-5 27. 4. O092400200029 30. 78. 1.63E-4 3.73E-5 11. 3. O092400200030 30. 79. 4.63E-5 8.96E-6 3.1 0.6 O092400200031 31. 76. 4.31E-4 1.42E-4 29. 10. O092400200032 31. 78. 0.00137 1.72E-4 92. 12. O092400200033 31. 79. 0.00143 2.57E-4 96. 17. O092400200034 31. 80. 3.87E-4 4.92E-5 26. 3. O092400200035 31. 81. 1.88E-4 7.76E-5 13. 5. O092400200036 32. 78. 0.00212 4.37E-4 140. 30. O092400200037 32. 79. 0.00298 4.33E-4 200. 30. O092400200038 32. 80. 0.0035 2.92E-4 234. 20. O092400200039 32. 81. 0.00525 5.61E-4 350. 40. O092400200040 32. 82. 0.00202 2.98E-4 135. 20. O092400200041 ENDDATA 23 0 O092400200042 ENDSUBENT 41 0 O092400299999 SUBENT O0924003 20140305 O052O092400300001 BIB 3 3 O092400300002 REACTION (92-U-238(P,F)ELEM/MASS,CUM,FY,,REL) O092400300003 STATUS (TABLE) tbl.1 from PL/B,405,230 O092400300004 HISTORY (20140305A) SD: SF6=PY -> FY in REACTION code. O092400300005 ENDBIB 3 0 O092400300006 NOCOMMON 0 0 O092400300007 DATA 4 12 O092400300008 ELEMENT MASS DATA DATA-ERR O092400300009 NO-DIM NO-DIM ARB-UNITS ARB-UNITS O092400300010 29. 71. 7.1 0.8 O092400300011 29. 72. 15. 3. O092400300012 29. 73. 10. 3. O092400300013 30. 74. 25. 4. O092400300014 30. 75. 69. 8. O092400300015 31. 76. 84. 8. O092400300016 32. 77. 155. 9. O092400300017 33. 78. 320. 60. O092400300018 33. 79. 460. 60. O092400300019 33. 80. 540. 60. O092400300020 33. 81. 790. 60. O092400300021 33. 82. 1530. 200. O092400300022 ENDDATA 14 0 O092400300023 ENDSUBENT 22 0 O092400399999 SUBENT O0924004 20140305 O052O092400400001 BIB 3 10 O092400400002 REACTION (92-U-238(P,F)ELEM,CHG,FY) O092400400003 Elemental yields (%) O092400400004 ANALYSIS Experimental elemental yields were obtained by GaussianO092400400005 fitting of the independent yields for the isotope O092400400006 chains of Cu, Zn, Ga and Ge. Due to the lack of O092400400007 experimental data, the value for Ni was estimated O092400400008 using the experimental yield of 71Ni only and the O092400400009 theoretical value of the average mass equal 71.23 O092400400010 and the mass dispersion equal 1.47, for the Ni-chain. O092400400011 HISTORY (20140305T) SD: Subent was added from D0149004. O092400400012 ENDBIB 10 0 O092400400013 NOCOMMON 0 0 O092400400014 DATA 2 5 O092400400015 ELEMENT DATA O092400400016 NO-DIM PC/FIS O092400400017 28. 0.034 O092400400018 29. 0.059 O092400400019 30. 0.26 O092400400020 31. 0.48 O092400400021 32. 1.84 O092400400022 ENDDATA 7 0 O092400400023 ENDSUBENT 22 0 O092400499999 ENDENTRY 4 0 O092499999999