ENTRY 41681 20191021 41864168100000001 SUBENT 41681001 20191021 41864168100100001 BIB 13 24 4168100100002 REFERENCE (J,PAN,58,1841,1995) Engl.translation of: 4168100100003 (J,YF,58,1948,1995) Issue 11 4168100100004 (J,PAN,56,24,1993) Engl.translation of: 4168100100005 (J,YF,56,40,1993) Issue 1 . 4168100100006 Prelim.data on fig.2a for Subent 002. 4168100100007 AUTHOR (A.A.Goverdovsky,V.F.Mitrofanov,V.A.Khryachkov) 4168100100008 TITLE Mass-energy distributions of fragments formed in 243Am 4168100100009 fission induced by fast neutrons 4168100100010 REL-REF (O,41682001,A.A.Goverdovskii,J,PAN,56,24,1993) 4168100100011 Data for U-236,238, Np-237 measured by Si-detectors 4168100100012 INSTITUTE (4RUSFEI) 4168100100013 FACILITY (VDG,4RUSFEI) Accelerator KG-2.5,IPPE 4168100100014 SAMPLE .Am-243 as oxide with thickness ~80 mug/cm2, on 4168100100015 Al(2)O(3) backing. 4168100100016 (95-AM-243,ENR=0.97) 4168100100017 .U-235 targets 4168100100018 DECAY-DATA (95-AM-243,7370.YR) 4168100100019 METHOD 2E-method 4168100100020 DETECTOR (SI) Silicon semiconductor detectors in coincidence. 4168100100021 Energy and mass resolution 1.5 - 2. % . 4168100100022 ASSUMED (ASSUM,92-U-235(N,F),,KE,LF+HF) 4168100100023 ANALYSIS U-235(N,F) primary mass distribution was used for 4168100100024 normalization. 4168100100025 HISTORY (20191021C) 4168100100026 ENDBIB 24 0 4168100100027 COMMON 1 3 4168100100028 ASSUM 4168100100029 MEV 4168100100030 170.6 4168100100031 ENDCOMMON 3 0 4168100100032 ENDSUBENT 31 0 4168100199999 SUBENT 41681002 20191021 41864168100200001 BIB 5 21 4168100200002 REACTION (95-AM-243(N,F)MASS,PRE,FY) 4168100200003 REL-REF (A,21545013,M.Asghar+,J,NP/A,334,(2),327,1980) 4168100200004 (R,,C.Wagemans+,R,JINR-E7-94-19,89,1994) Proc.Int. 4168100200005 Symp.on Dynamical Aspects of nuclear fission,Smolenice,4168100200006 Slovakia,1993, JINR,E7-94-19,1994, page 89 4168100200007 Data of M.Asghar+ and C.Wagemans+ are used for 4168100200008 comparison on Fig.1 4168100200009 ADD-RES Mass distribution was fitted by sum of Gaussians with 4168100200010 parameters: 4168100200011 - weights of 1st and 2nd standard, symmetrical and 4168100200012 unsymmetrical mass channels : 4168100200013 Y1, Y2, Ys, Yas (%) 4168100200014 18.3+-0.2 76.7+-0.9 1.0+-0.1 4.1+-0.2 4168100200015 - average mass for mentioned channels : 4168100200016 M1, M2, Ms, Mas 4168100200017 134.1+-0.6 140.2+-0.3 122. 154.7+-1.74168100200018 - root of dispersion : 4168100200019 SIGm1, SIGm2, SIGms, SIGmas 4168100200020 4.9+-0.2 7.0+-0.1 7.5+-3.0 6.1+-0.5 4168100200021 ERR-ANALYS Quantization error on scale Y - 0.05 %/fis 4168100200022 STATUS (CURVE) Fig.1 of Yad.Fiz.,v.58,p.1948,1995 4168100200023 ENDBIB 21 0 4168100200024 COMMON 2 3 4168100200025 EN ERR-DIG 4168100200026 MEV PC/FIS 4168100200027 1. 0.012 4168100200028 ENDCOMMON 3 0 4168100200029 DATA 2 44 4168100200030 MASS DATA 4168100200031 NO-DIM PC/FIS 4168100200032 122. 0.333 4168100200033 123. 0.386 4168100200034 124. 0.547 4168100200035 125. 0.697 4168100200036 126. 0.955 4168100200037 127. 1.278 4168100200038 128. 1.709 4168100200039 129. 2.139 4168100200040 130. 2.635 4168100200041 131. 3.163 4168100200042 132. 3.670 4168100200043 133. 3.928 4168100200044 134. 4.380 4168100200045 135. 4.768 4168100200046 136. 5.177 4168100200047 137. 5.370 4168100200048 138. 5.315 4168100200049 139. 5.335 4168100200050 140. 5.193 4168100200051 141. 5.095 4168100200052 142. 4.770 4168100200053 143. 4.466 4168100200054 144. 4.141 4168100200055 145. 3.772 4168100200056 146. 3.306 4168100200057 147. 3.003 4168100200058 148. 2.440 4168100200059 149. 2.201 4168100200060 150. 1.876 4168100200061 151. 1.680 4168100200062 152. 1.344 4168100200063 153. 1.234 4168100200064 154. 0.920 4168100200065 155. 0.821 4168100200066 156. 0.647 4168100200067 157. 0.527 4168100200068 158. 0.450 4168100200069 159. 0.417 4168100200070 160. 0.264 4168100200071 161. 0.230 4168100200072 162. 0.208 4168100200073 163. 0.163 4168100200074 164. 0.194 4168100200075 165. 0.128 4168100200076 ENDDATA 46 0 4168100200077 ENDSUBENT 76 0 4168100299999 ENDENTRY 2 0 4168199999999