ENTRY O1009 20200817 O079O100900000001 SUBENT O1009001 20200817 O079O100900100001 BIB 12 21 O100900100002 TITLE Independent yields of neutron-rich nuclei in charged- O100900100003 particle induced fission. O100900100004 AUTHOR (M.Huhta, P.Dendooven, A.Honkanen, G.Lhersonneau, O100900100005 M.Oinonen, H.Penttila, K.Perajarvi, V.Rubchenya, O100900100006 J.Aysto) O100900100007 INSTITUTE (2SF JYV) O100900100008 REFERENCE (J,NIM/B,126,201,1997) O100900100009 FACILITY (CYCLO,2SF JYV) The on-line mass separator IGISOL. O100900100010 INC-SOURCE (ISOL) ISOLDE Separator. O100900100011 SAMPLE The 15 mg/cm**2 thick natural uranium target and O100900100012 natural thorium target with a 50-MeV H2+ beam of 3 muA O100900100013 intensity, were used. O100900100014 ADD-RES (COMP) The theoretical model for calculating mass and O100900100015 independent fission products. O100900100016 METHOD (OLMS,ACTIV,BCINT) O100900100017 ERR-ANALYS (DATA-ERR) No information about source of uncertainty O100900100018 STATUS (CURVE) fig.3 from Nucl.Instr.Meth.,B126(1997)201 O100900100019 HISTORY (20021021C) O100900100020 (20030515U) Last checking has been done. O100900100021 (20200817A) SD: Subents 002,003 deleted (not for EXFOR:O100900100022 Intensity is given in atoms/sec (suspicious data)). O100900100023 ENDBIB 21 0 O100900100024 COMMON 1 3 O100900100025 EN O100900100026 MEV O100900100027 25. O100900100028 ENDCOMMON 3 0 O100900100029 ENDSUBENT 28 0 O100900199999 NOSUBENT O1009002 20200817 O079O100900200001 NOSUBENT O1009003 20200817 O079O100900300001 SUBENT O1009004 20200817 O079O100900400001 BIB 5 16 O100900400002 REACTION (92-U-0(P,X)ELEM/MASS,,SIG) O100900400003 DETECTOR (LONGC) The neutron long-counter consisted of 42 3-He O100900400004 ionization chamber tubes, which were arranged in two O100900400005 concentering rings in a polyethylene block. O100900400006 REL-REF (N,O0499001,P.P.Jauho+,J,PR/C,49,2036,1994) O100900400007 Theoretical models. O100900400008 COMMENT -By authors. Available experimental values are O100900400009 normalized to these predictions by setting the sum of O100900400010 the corresponding theoretical cross sections. The O100900400011 separation efficiencies for different isotopes of a O100900400012 given element are assumed to be equal. One can see thatO100900400013 the neutron-rich slopes of experimental isotopes O100900400014 distributions are described quite well. Although, no O100900400015 experimentally observed odd-even fluctuations are O100900400016 reproduced. O100900400017 HISTORY (20200817U) SD: PART-DET deleted. ERR-T -> DATA-ERR. O100900400018 ENDBIB 16 0 O100900400019 COMMON 1 3 O100900400020 ERR-DIG O100900400021 PER-CENT O100900400022 5. O100900400023 ENDCOMMON 3 0 O100900400024 DATA 4 26 O100900400025 ELEMENT MASS DATA DATA-ERR O100900400026 NO-DIM NO-DIM MB PER-CENT O100900400027 39. 99. 16. O100900400028 39. 100. 5.7 O100900400029 39. 101. 2.11 O100900400030 39. 102. 0.533 O100900400031 39. 103. 5.6E-02 30. O100900400032 41. 105. 6.6 O100900400033 41. 106. 2.34 O100900400034 41. 107. 0.547 7. O100900400035 41. 108. 0.16 25. O100900400036 41. 109. 2.1E-02 60. O100900400037 41. 110. 4.5E-03 60. O100900400038 43. 111. 2.11 O100900400039 43. 112. 0.75 7. O100900400040 50. 127. 23.6 O100900400041 50. 128. 7.8 7. O100900400042 50. 130. 2.6 19. O100900400043 50. 131. 0.76 11. O100900400044 50. 132. 0.442 7. O100900400045 50. 133. 1.7E-02 50. O100900400046 51. 130. 20.1 8. O100900400047 51. 131. 17.2 7. O100900400048 51. 132. 6.9 O100900400049 51. 133. 2.03 15. O100900400050 51. 134. 0.7 6. O100900400051 52. 133. 27.1 O100900400052 52. 134. 10.4 O100900400053 ENDDATA 28 0 O100900400054 ENDSUBENT 53 0 O100900499999 ENDENTRY 4 0 O100999999999