ENTRY 23675 20251218 SUBENT 23675001 20251218 BIB 15 123 2367500100002 TITLE New insights on fission of 235U induced by high 2367500100003 energy neutrons from a new measurement at nTOF 2367500100004 AUTHOR (A.Manna, E.Pirovano, P.Console Camprini, L.Cosentino, 2367500100005 M.Dietz, Q.Ducasse, P.Finocchiaro, C.Le Naour, 2367500100006 D.Mancusi, C.Massimi, A.Mengoni, R.Nolte, D.Radeck, 2367500100007 L.Tassan-Got, N.Terranova, G.Vannini, A.Ventura, 2367500100008 O.Aberle, V.Alcayne, S.Amaducci, J.Andrzejewski, 2367500100009 L.Audouin, V.Babiano-Suarez, M.Bacak, M.Barbagallo, 2367500100010 S.Bennett, E.Berthoumieux, J.Billowes, D.Bosnar, 2367500100011 A.Brown, M.Busso, M.Caamano, L.Caballero-Ontanaya, 2367500100012 F.Calvino, M.Calviani, D.Cano-Ott, A.Casanovas, 2367500100013 D.M.Castelluccio, F.Cerutti, E.Chiaveri, N.Colonna, 2367500100014 G.Cortes, M.A.Cortes-Giraldo, S.Cristallo, L.A.Damone,2367500100015 P.J.Davies, M.Diakaki, C.Domingo-Pardo, R.Dressler, 2367500100016 E.Dupont, I.Duran, Z.Eleme, B.Fernandez-Dominguez, 2367500100017 A.Ferrari, V.Furman, K.Goebel, R.Garg, 2367500100018 A.Gawlik-Ramiega, S.Gilardoni, I.F.Goncalves, 2367500100019 E.Gonzalez-Romero, C.Guerrero, F.Gunsing, H.Harada, 2367500100020 S.Heinitz, J.Heyse, D.G.Jenkins, A.Junghans, 2367500100021 F.Kaeppeler, Y.Kadi, A.Kimura, I.Knapova, M.Kokkoris, 2367500100022 Y.Kopatch, M.Krticka, D.Kurtulgil, I.Ladarescu, 2367500100023 C.Lederer-Woods, H.Leeb, J.Lerendegui-Marco, 2367500100024 S.J.Lonsdale, D.Macina, T.Martinez, A.Masi, P.Mastinu,2367500100025 M.Mastromarco, E.A.Maugeri, A.Mazzone, E.Mendoza, 2367500100026 V.Michalopoulou, P.M.Milazzo, F.Mingrone, 2367500100027 J.Moreno-Soto, A.Musumarra, A.Negret, F.Ogallar, 2367500100028 A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, C.Petrone,2367500100029 L.Piersanti, I.Porras, J.Praena, J.M.Quesada, 2367500100030 D.Ramos-Doval, T.Rauscher, R.Reifarth, D.Rochman, 2367500100031 C.Rubbia, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx,2367500100032 D.Schumann, A.Sekhar, A.G.Smith, N.V.Sosnin, P.Sprung,2367500100033 A.Stamatopoulos, G.Tagliente, J.L.Tain, 2367500100034 A.Tarifeno-Saldivia, Th.Thomas, P.Torres-Sanchez, 2367500100035 A.Tsinganis, J.Ulrich, S.Urlass, S.Valenta, V.Variale,2367500100036 P.Vaz, D.Vescovi, V.Vlachoudis, R.Vlastou, A.Wallner, 2367500100037 P.J.Woods, T.Wright, P.Zugec) 2367500100038 INSTITUTE (2ITYUBO,2GERPTB,2ITYBOL,2ITYLNS,2UK EDG,2FR PAR, 2367500100039 2FR SAC,2ZZZCER,2GRCTUA,2ITYEFR,2SPNPCM,2ITYCAT, 2367500100040 3POLLOU,2SPNVAL,2AUSATI,2ITYBAU,2UK MAN,3CROZAG, 2367500100041 2UK YRK,2ITYUPG,2SPNSAU,2SPNUPC,2SPNSEU,2ITYOAC, 2367500100042 2SWTPSI,2GRCIOA,2GERFRK,2PRTLFE,2JPNJAE,2ZZZGEL, 2367500100043 2GERZFK,2GERKFK,3CZRCHU,2ITYPAD,2ITYTRI,3RUMBUC, 2367500100044 2SPNGRU,2AUSVIE,2SWTBAS,2UK HFS,3INDTRM,3AULCBR) 2367500100045 (2ITYITY) Consiglio Nazionale delle Ricerche, Bari 2367500100046 REFERENCE (J,PL/B,860,139213,2025) 2367500100047 REL-REF (I,,E.Pirovano+,J,JINS,18,P11011,2023) 2367500100048 Details on PPFC+RPT measurements 2367500100049 (I,,A.Manna+,J,JINS,18,P04024,2023) 2367500100050 Details on PPAC+RPT measurements 2367500100051 FACILITY (SYNCY,2ZZZCER) CERN nTOF facility. 2367500100052 Protons (7 to 8.5E+12 protons/pulse, pulse width of 2367500100053 7 nsec) were accelerated to 20 GeV/c with repetition 2367500100054 rate of 0.8 Hz at maximum. 2367500100055 INC-SOURCE (SPALL) 1E+6 neutrons/pulse were produced in a Pb 2367500100056 spallation target coupled to water moderators. 2367500100057 The diameter of the neutron beam at sample position 2367500100058 is 2 cm. 2367500100059 INC-SPECT (EN-RSL-HW) Half of bin width 2367500100060 SAMPLE Two 235U (92.699(5)%) and eight 235U (99.933(14)%) 2367500100061 enriched samples mounted in PPFC and PPAC. 2367500100062 Two polyethylene sheets for n-p scattering measurement.2367500100063 METHOD (TOF) Flight path of 185 m 2367500100064 (EDE) for separation of (n,p) events form (n,d), (n,t) 2367500100065 and (n,a) events 2367500100066 CORRECTION Corrected for 12C(n,p) events by an additional 2367500100067 measurement using graphite samples 2367500100068 MONITOR (1-H-1(N,EL)1-H-1,,DA,P) 2367500100069 n-p scattering cross section in the centre-of-mass 2367500100070 system for proton at 20 and 25 deg in the laboratory 2367500100071 system in LA150 library (VL40 wave analysis energy 2367500100072 dependent phase-shift solution of Arndt above 26 MeV) 2367500100073 interpolated by MCNP 2367500100074 +----------------------------------------------------+ 2367500100075 Tlab (MeV) sigma,cm (mb/sr) 2367500100076 theta,lab=20.0 deg theta,lab=25.0 deg 2367500100077 ------------------------------------------------------ 2367500100078 20.0 151.1773 143.0919 2367500100079 25.0 119.6774 112.3854 2367500100080 30.0 98.2831 91.4940 2367500100081 35.0 82.9424 76.5152 2367500100082 40.0 71.5839 65.3763 2367500100083 45.0 62.8253 56.8485 2367500100084 50.0 55.9827 50.1418 2367500100085 55.0 50.5020 44.8111 2367500100086 60.0 46.0731 40.4603 2367500100087 65.0 42.4019 36.9134 2367500100088 70.0 39.3703 33.9688 2367500100089 75.0 36.8074 31.5020 2367500100090 80.0 34.6420 29.4214 2367500100091 85.0 32.7947 27.6482 2367500100092 90.0 31.2097 26.1335 2367500100093 95.0 29.8372 24.8245 2367500100094 100.0 28.6440 23.6949 2367500100095 110.0 26.6841 21.8386 2367500100096 120.0 25.1544 20.3961 2367500100097 130.0 23.9333 19.2479 2367500100098 140.0 22.9368 18.3085 2367500100099 150.0 22.1063 17.5243 2367500100100 160.0 21.3968 16.8537 2367500100101 170.0 20.7786 16.2632 2367500100102 180.0 20.2285 15.7369 2367500100103 190.0 19.7309 15.2568 2367500100104 200.0 19.2700 14.8089 2367500100105 210.0 18.8391 14.3918 2367500100106 220.0 18.4333 13.9956 2367500100107 230.0 18.0407 13.6170 2367500100108 240.0 17.6676 13.2522 2367500100109 250.0 17.3040 12.8977 2367500100110 260.0 16.9518 12.5551 2367500100111 270.0 16.6048 12.2189 2367500100112 280.0 16.2674 11.8915 2367500100113 290.0 15.9355 11.5723 2367500100114 300.0 15.6067 11.2609 2367500100115 310.0 15.2859 10.9539 2367500100116 320.0 14.9683 10.6510 2367500100117 330.0 14.6563 10.3578 2367500100118 340.0 14.3475 10.0676 2367500100119 350.0 14.0429 9.7806 2367500100120 +----------------------------------------------------+ 2367500100121 MONIT-REF (,R.A.Arndt,S,NEANDC-305,39,1991) 2367500100122 STATUS (APRVD) Proofread by Elisa Pirovano and Alice Manna (2025-12-23) HISTORY (20251218R) Data received from Elisa Pirovano 2367500100124 (20251218C) On+ED 2367500100125 ENDBIB 123 0 2367500100126 NOCOMMON 0 0 2367500100127 ENDSUBENT 126 0 2367500199999 SUBENT 23675002 20251218 BIB 6 129 2367500200002 REACTION 1(92-U-235(N,F),,SIG) PPFC+3S-RPT dataset 2367500200003 2(92-U-235(N,F),,SIG) PPAC+MSRPT dataset 2367500200004 DETECTOR 1.PPFC+3S-RPT dataset 2367500200005 (FISCH) Parallel Plate Fission Chamber (PPFC) 2367500200006 containing eight 235U samples (42 mm diam., 264 to 2367500200007 338 ug/cm2 determined by alpha counting), 2367500200008 for measurement up to 145 MeV. 2367500200009 (TELES,SCIN,SCIN) Recoil proton telescope 2367500200010 Triple-stage RPT (3S-RPT) at 25 deg 2367500200011 2.PPAC+MSRPT dataset 2367500200012 (PPAC) Parallel Plate Avalanche Counter containing 2367500200013 two 235U samples (80 mm diam., 263 ug/cm2 and 2367500200014 282 ug/cm2) 2367500200015 (TELES,SCIN,SCIN) Recoil proton telescope 2367500200016 . Multi-stage RPT (MS-RPTL) at 25 deg 2367500200017 . Multi-stage RPT (MS-RPTH) at 20 deg 2367500200018 COMMENT * By Alice Manna and Elisa Pirovano (2025-12-04): 2367500200019 1.PPFC+3S-RPT dataset 2367500200020 The cross section obtained with PPFC and 3S-RPT. In 2367500200021 this detection system, the recoil proton telescope 2367500200022 was at a proton emission angle theta,p of 25 deg. 2367500200023 In this case, the measured fission cross section is 2367500200024 proportional to the differential proton emission 2367500200025 cross section dsigma/dOmega,p at theta,p) in the 2367500200026 laboratory frame. 2367500200027 Therefore, it is possible to re-normalized it in 2367500200028 case of change of the neutron-proton elastic 2367500200029 scattering cross section at the corresponding neutron 2367500200030 scattering angle. 2367500200031 2.PPAC+MSRPT dataset 2367500200032 The cross section obtained with PPAC and MS-RPTL and 2367500200033 MS-RPTH. In this detection system two recoil proton 2367500200034 telescopes were used, positioned at 25 deg and 20 deg,2367500200035 respectively. 2367500200036 In this case the normalization is not straightforward, 2367500200037 therefore we are proposing a method (outlined in ????)2367500200038 for the re-normalization. 2367500200039 MISC-COL 2(MISC) [w(20 deg)*phi(20 deg)]/[w(25 deg)*phi(25 deg)] 2367500200040 ERR-ANALYS (ERR-T) Total uncertainty 2367500200041 (ERR-S) Statistical uncertainty 2367500200042 (ERR-SYS) Total systematic uncertainty 2367500200043 (ERR-2) Systematic uncertainty correlated between PPFC 2367500200044 and PPAC datasets: 2367500200045 . Isotopic composition of the PE samples (H/C ratio) 2367500200046 1.5% 2367500200047 . Areal density of the PE samples, correlated 2367500200048 component, depending on the sample used for each 2367500200049 energy interval 2367500200050 0.2%-0.8% 2367500200051 . Areal density of the C samples, correlated component,2367500200052 depending on the sample 2367500200053 0.3%-1.1% 2367500200054 . Beam profile 2367500200055 0.5% 2367500200056 . Beam transmission through PPFC, PPAC, energy 2367500200057 dependent 2367500200058 0.2%-0.5% 2367500200059 1(ERR-1) PPFC/3S-RPT systematic uncertainty uncorrelated2367500200060 with PPAC/MSR-RPTs systematic uncertainty: 2367500200061 . Isotopic composition of the uranium targets of the 2367500200062 PPFC 2367500200063 0.0014% 2367500200064 . Mass of the uranium targets of the PPFC 2367500200065 0.2% 2367500200066 . Correction on the effective areal density of the 2367500200067 uranium targets of the PPFC 2367500200068 0.6% 2367500200069 . Areal density of the PE samples, uncorrelated 2367500200070 component for the 3S-RPT, depending on the RPT 2367500200071 configuration used for each energy interval 2367500200072 0%-0.4% 2367500200073 . Areal density of the C samples, uncorrelated 2367500200074 component for the 3S-RPT, depending on the RPT 2367500200075 configuration 2367500200076 0%-0.9% 2367500200077 . PPFC detection efficiency: zero-bias efficiency, 2367500200078 weak energy dependence 2367500200079 1.0%-1.2% 2367500200080 . PPFC detection efficiency: extrapolation below 2367500200081 threshold 2367500200082 2.9% 2367500200083 . PPFC dead-time correction, energy dependent 0.04%-0.2% 2367500200086 . 3S-RPT angle 2367500200087 0.1%-0.6% 2367500200088 . 3S-RPT distance 2367500200089 0.8% 2367500200090 . 3S-RPT effective solid angle (area of the dEz 2367500200091 detector) 2367500200092 0.4%-0.7% 2367500200093 . 3S-RPT dead-time correction 2367500200094 0.6%-0.9% 2367500200095 . 3S-RPT: event selection in the dE-E 2367500200096 0.2%-0.4% 2367500200097 . 3S-RPT: efficiency calculation fit 2367500200098 2.4% 2367500200099 2(ERR-1) PPAC/MS-RPTs systematic uncertainty 2367500200100 uncorrelated with PPFC/3S-RPT systematic uncertainty: 2367500200101 . Mass of the uranium samples of the PPAC 2367500200102 1.0% 2367500200103 . Areal density of the PE samples, uncorrelated 2367500200104 component for the MS-RPTs, depending on the sample 2367500200105 used for each energy interval 2367500200106 0.0%-0.3% 2367500200107 . Areal density of the C samples, uncorrelated 2367500200108 component for the MS-RPTs, depending on the sample 2367500200109 0%-0.5% 2367500200110 . PPAC: reconstruction of the fission fragments 2367500200111 trajectories 2367500200112 0.4% 2367500200113 . PPAC efficiency calculation fit, energy dependent 2367500200114 2.0%-2.7% 2367500200115 . PPAC anisotropy correction, energy dependent 2367500200116 0%-1.2% 2367500200117 . MS-RPT position, depending on the RPT configuration 2367500200118 0.9%-1.2% 2367500200119 . MS-RPT signal reconstruction, depending on the RPT 2367500200120 detectors included in the analysis of each energy 2367500200121 interval 2367500200122 0.5%-1.8% 2367500200123 . MS-RPT: events selection in the dE-E matrix, 2367500200124 depending on the RPT detectors included in the 2367500200125 analysis 2367500200126 2.0%-5.0% 2367500200127 . MS-RPT dead-time correction, depending on the RPT 2367500200128 detectors included in the analysis 2367500200129 1.0%-2.0% 2367500200130 STATUS (TABLE,,A.Manna+,J,PL/B,860,139213,2025) ENDBIB 129 0 2367500200132 NOCOMMON 0 0 2367500200133 DATA 14 50 2367500200134 EN EN-RSL-HW DATA 1ERR-T 1ERR-S 1ERR-SYS 12367500200135 ERR-1 1DATA 2ERR-T 2ERR-S 2ERR-SYS 2ERR-1 22367500200136 ERR-2 MISC 2 2367500200137 MEV MEV MB MB MB MB 2367500200138 PER-CENT MB MB MB MB PER-CENT 2367500200139 PER-CENT NO-DIM 2367500200140 10.63 0.63 2367500200141 1795. 147. 88. 117. 6.5 2367500200142 0.000 2367500200143 11.95 0.70 2367500200144 1768. 137. 73. 116. 6.5 2367500200145 0.000 2367500200146 13.44 0.79 2367500200147 1887. 142. 71. 123. 6.5 2367500200148 0.000 2367500200149 15.12 0.89 2367500200150 2040. 152. 73. 133. 6.5 2367500200151 0.000 2367500200152 17.01 1.00 2367500200153 2094. 153. 69. 137. 6.5 2367500200154 0.000 2367500200155 19.14 1.13 2367500200156 1982. 140. 52. 130. 6.5 2367500200157 0.000 2367500200158 21.86 1.60 2367500200159 2112. 147. 50. 138. 6.5 2367500200160 0.000 2367500200161 25.30 1.85 2367500200162 2134. 149. 53. 140. 6.5 2367500200163 0.000 2367500200164 29.22 0.71 2175. 125. 76. 99. 2367500200165 4.5 2367500200166 2367500200167 30.68 0.75 2131. 121. 73. 97. 2367500200168 4.5 2367500200169 2367500200170 32.21 0.79 2158. 123. 74. 98. 2367500200171 4.5 2367500200172 2367500200173 33.82 0.83 2174. 113. 51. 101. 2367500200174 4.6 2367500200175 2367500200176 35.51 0.87 2087. 108. 49. 97. 2367500200177 4.6 2367500200178 2367500200179 37.29 0.91 2105. 110. 51. 97. 2367500200180 4.6 2367500200181 2367500200182 39.16 0.95 1987. 105. 50. 92. 2367500200183 4.1 2007. 102. 62. 81. 3.4 2367500200184 2.1 0.000 2367500200185 41.12 1.01 1968. 105. 51. 91. 2367500200186 4.1 1991. 104. 67. 80. 3.4 2367500200187 2.1 0.000 2367500200188 43.17 1.05 1962. 106. 54. 91. 2367500200189 4.1 1925. 102. 66. 77. 3.4 2367500200190 2.1 0.000 2367500200191 45.33 1.11 2025. 104. 43. 94. 2367500200192 4.1 1972. 104. 67. 79. 3.4 2367500200193 2.1 0.000 2367500200194 47.59 1.16 2034. 105. 47. 94. 2367500200195 4.1 1874. 101. 67. 75. 3.4 2367500200196 2.1 0.000 2367500200197 49.97 1.22 1880. 98. 45. 87. 2367500200198 4.1 1916. 103. 68. 77. 3.4 2367500200199 2.1 0.000 2367500200200 52.73 1.54 1946. 100. 43. 90. 2367500200201 4.2 1826. 94. 62. 71. 3.4 2367500200202 1.9 0.000 2367500200203 55.89 1.63 1894. 99. 45. 88. 2367500200204 4.2 1847. 90. 53. 72. 3.4 2367500200205 1.9 0.000 2367500200206 59.25 1.73 1870. 99. 48. 87. 2367500200207 4.2 1797. 88. 53. 70. 3.4 2367500200208 1.9 0.000 2367500200209 62.80 1.83 1829. 99. 51. 85. 2367500200210 4.2 1800. 89. 54. 71. 3.4 2367500200211 1.9 0.000 2367500200212 66.57 1.94 1805. 100. 53. 84. 2367500200213 4.2 1744. 87. 54. 68. 3.4 2367500200214 1.9 0.000 2367500200215 70.57 2.06 1769. 99. 55. 83. 2367500200216 4.3 1697. 85. 54. 66. 3.4 2367500200217 1.9 0.000 2367500200218 74.80 2.18 1717. 99. 58. 80. 2367500200219 4.3 1696. 86. 55. 66. 3.4 2367500200220 1.9 0.000 2367500200221 79.28 2.31 1761. 103. 63. 82. 2367500200222 4.3 1642. 84. 54. 64. 3.4 2367500200223 1.9 0.000 2367500200224 84.04 2.45 1697. 101. 62. 79. 2367500200225 4.3 1671. 81. 48. 65. 3.4 2367500200226 1.9 2.180 2367500200227 89.09 2.60 1685. 105. 70. 79. 2367500200228 4.3 1632. 79. 46. 64. 3.4 2367500200229 1.9 5.072 2367500200230 94.43 2.75 1586. 100. 66. 74. 2367500200231 4.3 1627. 79. 47. 64. 3.4 2367500200232 1.9 6.778 2367500200233 100.10 2.92 1569. 107. 79. 72. 2367500200234 4.2 1707. 82. 48. 67. 3.4 2367500200235 1.9 5.915 2367500200236 106.62 3.61 1591. 127. 105. 72. 2367500200237 4.2 1602. 77. 44. 63. 3.5 2367500200238 1.7 12.657 2367500200239 114.08 3.86 1516. 125. 104. 69. 2367500200240 4.2 1540. 75. 44. 61. 3.6 2367500200241 1.7 13.809 2367500200242 122.06 4.13 1498. 135. 116. 68. 2367500200243 4.2 1528. 75. 45. 61. 3.6 2367500200244 1.7 4.796 2367500200245 130.61 4.42 1454. 122. 102. 66. 2367500200246 4.2 1523. 76. 46. 61. 3.6 2367500200247 1.7 4.143 2367500200248 139.75 4.72 1498. 131. 111. 69. 2367500200249 4.2 1442. 72. 43. 58. 3.6 2367500200250 1.7 2.360 2367500200251 149.53 5.06 2367500200252 1519. 75. 44. 61. 4.0 2367500200253 4.163 2367500200254 161.55 6.96 2367500200255 1535. 74. 41. 62. 4.0 2367500200256 3.959 2367500200257 176.08 7.58 2367500200258 1396. 70. 40. 57. 4.1 2367500200259 3.600 2367500200260 191.93 8.27 2367500200261 1505. 75. 43. 62. 4.1 2367500200262 3.540 2367500200263 209.20 9.01 2367500200264 1523. 78. 46. 63. 4.2 2367500200265 3.545 2367500200266 228.03 9.82 2367500200267 1448. 75. 45. 60. 4.2 2367500200268 3.531 2367500200269 248.56 10.71 2367500200270 1453. 75. 46. 60. 4.1 2367500200271 1.940 2367500200272 270.93 11.67 2367500200273 1407. 74. 46. 58. 4.1 2367500200274 1.804 2367500200275 295.31 12.72 2367500200276 1579. 84. 53. 65. 4.1 2367500200277 2.162 2367500200278 321.88 13.86 2367500200279 1378. 75. 48. 57. 4.2 2367500200280 1.886 2367500200281 350.85 15.11 2367500200282 1501. 83. 54. 63. 4.2 2367500200283 2.069 2367500200284 384.26 18.30 2367500200285 1620. 90. 59. 68. 4.2 2367500200286 1.941 2367500200287 422.69 20.13 2367500200288 1481. 84. 55. 63. 4.2 2367500200289 2.074 2367500200290 ENDDATA 156 0 2367500200291 ENDSUBENT 290 0 2367500299999 SUBENT 23675003 20251218 BIB 6 29 2367500300002 REACTION (92-U-235(N,F),,SIG,,AV) 2367500300003 ANALYSIS Weighted average of PPFC/3SRPT and PPAC/MSRPT datasets 2367500300004 MISC-COL Weights used to calculated the weighted mean 2367500300005 (MISC1) w(PPFC/3S-RPT) 2367500300006 (MISC2) w(PPAC/MS-RPTL) 2367500300007 ERR-ANALYS (DATA-ERR) The uncertainty results from the procedure to calculate the weighted average. COMMENT * By Alice Manna and Elisa Pirovano (2025-12-04): 2367500300009 The final cross section obtained as weighted average 2367500300010 of the two independent results (in which we have a 2367500300011 contribution from both the neutron-proton elastic 2367500300012 scattering differential cross section). 2367500300013 This data set contains the weights used to calculate 2367500300014 the weighted mean, which makes it possible to 2367500300015 re-calculate the weighted mean of the re-normalized 2367500300016 fission cross sections measured with the two 2367500300017 experimental configurations PPFC/3S-RPT and 2367500300018 PPAC/MS-RPTL(H). 2367500300019 As discussed in E.Pirovano et al. "Absolute cross 2367500300020 section for neutron-induced fission of 235U in the 2367500300021 energy range from 10 MeV to 400 MeV" (to be published 2367500300022 in Phys.Rev.C and arXiv), these two data sets are 2367500300023 partially correlated, as the same polyethylene 2367500300024 samples and beam intensity monitors were employed. 2367500300025 However, a small re-normalization of the differential 2367500300026 neutron-proton scattering cross section will not 2367500300027 effect the stated relative uncertainty of the final 2367500300028 fission cross section. 2367500300029 STATUS (TABLE,,A.Manna+,J,PL/B,860,139213,2025) (DEP,23675002) Datasets from PPFC/3SRPT and PPAC/MSRPT 2367500300031 ENDBIB 29 0 2367500300032 NOCOMMON 0 0 2367500300033 DATA 6 50 2367500300034 EN EN-RSL-HW DATA DATA-ERR MISC1 MISC2 2367500300035 MEV MEV MB MB NO-DIM NO-DIM 2367500300036 10.63 0.63 1795. 147. 0. 1. 2367500300037 11.95 0.70 1768. 137. 0. 1. 2367500300038 13.44 0.79 1887. 142. 0. 1. 2367500300039 15.12 0.89 2040. 152. 0. 1. 2367500300040 17.01 1.00 2094. 153. 0. 1. 2367500300041 19.14 1.13 1982. 140. 0. 1. 2367500300042 21.86 1.60 2112. 147. 0. 1. 2367500300043 25.30 1.85 2134. 149. 0. 1. 2367500300044 29.22 0.71 2175. 125. 1. 0. 2367500300045 30.68 0.75 2131. 121. 1. 0. 2367500300046 32.21 0.79 2158. 123. 1. 0. 2367500300047 33.82 0.83 2174. 113. 1. 0. 2367500300048 35.51 0.87 2087. 108. 1. 0. 2367500300049 37.29 0.91 2105. 110. 1. 0. 2367500300050 39.16 0.95 1997. 79. 0.4828 0.5172 2367500300051 41.12 1.01 1980. 80. 0.4966 0.5034 2367500300052 43.17 1.05 1943. 79. 0.4793 0.5207 2367500300053 45.33 1.11 1999. 79. 0.5068 0.4932 2367500300054 47.59 1.16 1951. 79. 0.4816 0.5184 2367500300055 49.97 1.22 1897. 77. 0.5256 0.4744 2367500300056 52.73 1.54 1882. 73. 0.4703 0.5297 2367500300057 55.89 1.63 1868. 71. 0.4463 0.5537 2367500300058 59.25 1.73 1828. 70. 0.4314 0.5686 2367500300059 62.80 1.83 1813. 71. 0.4375 0.5625 2367500300060 66.57 1.94 1770. 70. 0.4248 0.5752 2367500300061 70.57 2.06 1727. 69. 0.4169 0.5831 2367500300062 74.80 2.18 1705. 69. 0.4206 0.5794 2367500300063 79.28 2.31 1688. 69. 0.3887 0.6113 2367500300064 84.04 2.45 1681. 67. 0.3769 0.6231 2367500300065 89.09 2.60 1650. 67. 0.3408 0.6592 2367500300066 94.43 2.75 1612. 65. 0.3686 0.6314 2367500300067 100.10 2.92 1658. 69. 0.3513 0.6487 2367500300068 106.62 3.61 1599. 68. 0.2514 0.7486 2367500300069 114.08 3.86 1534. 66. 0.2504 0.7496 2367500300070 122.06 4.13 1521. 67. 0.221 0.779 2367500300071 130.61 4.42 1505. 66. 0.2628 0.7372 2367500300072 139.75 4.72 1454. 65. 0.2177 0.7823 2367500300073 149.53 5.06 1519. 75. 0. 1. 2367500300074 161.55 6.96 1535. 74. 0. 1. 2367500300075 176.08 7.58 1396. 70. 0. 1. 2367500300076 191.93 8.27 1505. 75. 0. 1. 2367500300077 209.20 9.01 1523. 78. 0. 1. 2367500300078 228.03 9.82 1448. 75. 0. 1. 2367500300079 248.56 10.71 1453. 75. 0. 1. 2367500300080 270.93 11.67 1407. 74. 0. 1. 2367500300081 295.31 12.72 1579. 84. 0. 1. 2367500300082 321.88 13.86 1378. 75. 0. 1. 2367500300083 350.85 15.11 1501. 83. 0. 1. 2367500300084 384.26 18.30 1620. 90. 0. 1. 2367500300085 422.69 20.13 1481. 84. 0. 1. 2367500300086 ENDDATA 52 0 2367500300087 ENDSUBENT 86 0 2367500399999 SUBENT 23675004 20251218 BIB 4 6 2367500400002 REACTION (92-U-235(N,F),,SIG,,AV,DERIV) 2367500400003 ANALYSIS Averaged data processed by smoothing filter. The smoothed data starts from 149 MeV, below this energy the averaged cross section is reported. ERR-ANALYS (DATA-ERR) The uncertainty on the smoothed data results from the fitting procedure. STATUS (TABLE,,A.Manna+,J,PL/B,860,139213,2025) U5vsnp-smo (DEP,23675003) Averaged cross section 2367500400008 ENDBIB 6 0 2367500400009 NOCOMMON 0 0 2367500400010 DATA 4 50 2367500400011 EN EN-RSL-HW DATA DATA-ERR 2367500400012 MEV MEV MB MB 2367500400013 10.63 0.63 1795. 147. 2367500400014 11.95 0.70 1768. 137. 2367500400015 13.44 0.79 1887. 142. 2367500400016 15.12 0.89 2040. 152. 2367500400017 17.01 1.00 2094. 153. 2367500400018 19.14 1.13 1982. 140. 2367500400019 21.86 1.60 2112. 147. 2367500400020 25.30 1.85 2134. 149. 2367500400021 29.22 0.71 2175. 125. 2367500400022 30.68 0.75 2131. 121. 2367500400023 32.21 0.79 2158. 123. 2367500400024 33.82 0.83 2174. 113. 2367500400025 35.51 0.87 2087. 108. 2367500400026 37.29 0.91 2105. 110. 2367500400027 39.16 0.95 1997. 79. 2367500400028 41.12 1.01 1980. 80. 2367500400029 43.17 1.05 1943. 79. 2367500400030 45.33 1.11 1999. 79. 2367500400031 47.59 1.16 1951. 79. 2367500400032 49.97 1.22 1897. 77. 2367500400033 52.73 1.54 1882. 73. 2367500400034 55.89 1.63 1868. 71. 2367500400035 59.25 1.73 1828. 70. 2367500400036 62.80 1.83 1813. 71. 2367500400037 66.57 1.94 1770. 70. 2367500400038 70.57 2.06 1727. 69. 2367500400039 74.80 2.18 1705. 69. 2367500400040 79.28 2.31 1688. 69. 2367500400041 84.04 2.45 1681. 67. 2367500400042 89.09 2.60 1650. 67. 2367500400043 94.43 2.75 1612. 65. 2367500400044 100.10 2.92 1658. 69. 2367500400045 106.62 3.61 1599. 68. 2367500400046 114.08 3.86 1534. 66. 2367500400047 122.06 4.13 1521. 67. 2367500400048 130.61 4.42 1505. 66. 2367500400049 139.75 4.72 1454. 65. 2367500400050 149.53 5.06 1498. 21. 2367500400051 161.55 6.96 1486. 22. 2367500400052 176.08 7.58 1475. 22. 2367500400053 191.93 8.27 1468. 22. 2367500400054 209.20 9.01 1464. 22. 2367500400055 228.03 9.82 1464. 23. 2367500400056 248.56 10.71 1466. 24. 2367500400057 270.93 11.67 1470. 26. 2367500400058 295.31 12.72 1475. 29. 2367500400059 321.88 13.86 1480. 31. 2367500400060 350.85 15.11 1485. 32. 2367500400061 384.26 18.30 1489. 37. 2367500400062 422.69 20.13 1490. 55. 2367500400063 ENDDATA 52 0 2367500400064 ENDSUBENT 63 0 2367500499999 ENDENTRY 4 0 2367599999999