ENTRY A0229 20160317 A084A022900000001 SUBENT A0229001 20160317 A084A022900100001 BIB 7 13 A022900100002 TITLE The production of neutron-rich nuclides in the A022900100003 heavy-element region via He-3 induced reactions. A022900100004 AUTHOR (Y.Y.Chu,M.L.Zhou) A022900100005 REFERENCE (J,IRE,30,(2),1149,1983) A022900100006 INSTITUTE (1USABNL) A022900100007 (3CPRSIU) A022900100008 FACILITY (ISOCY,1USABNL) A022900100009 METHOD (CHSEP,BCINT,SITA) Additional information is absent. A022900100010 HISTORY (19841012C) A022900100011 (19861204U) A022900100012 (20160317A) SD:Updated to new date formats,lower case. A022900100013 Corrections in REACTION code in Subents 002-004.RAD-DETA022900100014 deleted from Subents (info presented in DECAY-DATA). A022900100015 ENDBIB 13 0 A022900100016 NOCOMMON 0 0 A022900100017 ENDSUBENT 16 0 A022900199999 SUBENT A0229002 20160317 A084A022900200001 BIB 7 17 A022900200002 REACTION (92-U-238(HE3,X)90-TH-233,,SIG,,(A)) A022900200003 DETECTOR (GELI) Ge(Li) detector (50 cm3 in size with FWHM of A022900200004 2.0 keV at 1332 keV) A022900200005 SAMPLE Uranium oxide of two different thickness and A022900200006 uranium foil (thickness - 0.0015 inch) were A022900200007 used in this measurement. A022900200008 DECAY-DATA (90-TH-233,22.2MIN,DG,162.0,0.0031, A022900200009 DG,169.0,0.0034, A022900200010 DG,459.4,0.0135, A022900200011 DG,670.1,0.0065) A022900200012 ERR-ANALYS (DATA-ERR) The errors of the cross sections reflect theA022900200013 larger quantity of either the combination of counting A022900200014 statistics, detector efficiency and chemical yield A022900200015 uncertainties or the standard deviation of the A022900200016 individual measurements from the mean. A022900200017 STATUS (TABLE) Tbl. 2 from IRE,30,(2),1149,1983 A022900200018 HISTORY (20160317A) SD: SF3=2A -> X in REACTION code. A022900200019 ENDBIB 17 0 A022900200020 NOCOMMON 0 0 A022900200021 DATA 3 3 A022900200022 EN DATA DATA-ERR A022900200023 MEV MICRO-B MICRO-B A022900200024 46.3 1.3 0.2 A022900200025 53.0 3.8 0.5 A022900200026 59.6 6.3 0.6 A022900200027 ENDDATA 5 0 A022900200028 ENDSUBENT 27 0 A022900299999 SUBENT A0229003 20160317 A084A022900300001 BIB 7 15 A022900300002 REACTION (92-U-238(HE3,X)90-TH-231,,SIG,,A) A022900300003 DETECTOR (GELI) Ge(Li) detector (50 cm3 in size with FWHM of A022900300004 2.0 keV at 1332 keV) A022900300005 SAMPLE Uranium oxide of two different thickness and A022900300006 uranium foil (thickness - 0.0015 inch) were A022900300007 used in this measurement. A022900300008 DECAY-DATA (90-TH-231,25.5HR,DG,84.5,0.065, A022900300009 DG,163.0,0.0016) A022900300010 ERR-ANALYS (DATA-ERR) The errors of the cross sections reflect theA022900300011 larger quantity of either the combination of counting A022900300012 statistics, detector efficiency and chemical yield A022900300013 uncertainties or the standard deviation of the A022900300014 individual measurements from the mean. A022900300015 STATUS (TABLE) Tbl. 2 from IRE,30,(2),1149,1983 A022900300016 HISTORY (20160317A) SD: SF3=2N+2A -> X in REACTION code. A022900300017 ENDBIB 15 0 A022900300018 NOCOMMON 0 0 A022900300019 DATA 3 3 A022900300020 EN DATA DATA-ERR A022900300021 MEV MICRO-B MICRO-B A022900300022 46.3 2.8 0.3 A022900300023 53.0 10.6 1.1 A022900300024 59.6 16.2 2.0 A022900300025 ENDDATA 5 0 A022900300026 ENDSUBENT 25 0 A022900399999 SUBENT A0229004 20160317 A084A022900400001 BIB 7 22 A022900400002 DETECTOR (PROPC) A022900400003 REACTION (92-U-238(HE3,X)89-AC-233,,SIG,,,DERIV) A022900400004 DECAY-DATA (90-TH-233,22.3MIN,B-) The authors attempted to observeA022900400005 Ac-233 by assaying the thorium samples into which A022900400006 the actinium has decayed. A022900400007 ((1.)89-AC-233-G,60.SEC) A022900400008 ((2.)89-AC-233-G,80.SEC) A022900400009 ((3.)89-AC-233-G,100.SEC) A022900400010 ((4.)89-AC-233-G,120.SEC) A022900400011 ((5.)89-AC-233-G,140.SEC) A022900400012 ((6.)89-AC-233-G,160.SEC) A022900400013 ((7.)89-AC-233-G,180.SEC) A022900400014 ((8.)89-AC-233-G,1332.SEC) A022900400015 COMMENT (By authors). In the data section the authors A022900400016 give calculated apparent cross sections for Ac-233 A022900400017 based on the observed Th-233 activities and different A022900400018 values assumed for the half-life of Ac-233. A022900400019 MISC-COL Number of series of experiment. A022900400020 STATUS (TABLE) Tbl. 3 from IRE,30,(2),1149,1983 A022900400021 HISTORY (20160317A) SD: SF3=B-8 -> X, SF9=CALC -> DERIV in A022900400022 REACTION code. HALF-LIFE and HL col. deleted, A022900400023 information moved to DECAY-DATA and DECAY-FLAG. A022900400024 ENDBIB 22 0 A022900400025 COMMON 1 3 A022900400026 EN A022900400027 MEV A022900400028 61. A022900400029 ENDCOMMON 3 0 A022900400030 DATA 3 32 A022900400031 DATA DECAY-FLAG MISC A022900400032 MICRO-B NO-DIM NO-DIM A022900400033 16.8 1. 3. A022900400034 93.4 1. 1. A022900400035 11.6 1. 4. A022900400036 28.4 1. 2. A022900400037 6.8 2. 3. A022900400038 4.6 2. 4. A022900400039 35. 2. 1. A022900400040 8.6 2. 2. A022900400041 3.8 3. 3. A022900400042 4.1 3. 2. A022900400043 2.6 3. 4. A022900400044 18.9 3. 1. A022900400045 1.8 4. 4. A022900400046 2.5 4. 3. A022900400047 12.4 4. 1. A022900400048 2.5 4. 2. A022900400049 1.7 5. 2. A022900400050 1.8 5. 3. A022900400051 9.1 5. 1. A022900400052 1.3 5. 4. A022900400053 1.4 6. 3. A022900400054 1.3 6. 2. A022900400055 1.1 6. 4. A022900400056 7.2 6. 1. A022900400057 1.2 7. 3. A022900400058 6.0 7. 1. A022900400059 1.1 7. 2. A022900400060 0.9 7. 4. A022900400061 1.5 8. 1. A022900400062 0.26 8. 3. A022900400063 0.26 8. 4. A022900400064 0.23 8. 2. A022900400065 ENDDATA 34 0 A022900400066 ENDSUBENT 65 0 A022900499999 ENDENTRY 4 0 A022999999999