ENTRY A1120 19990319 0000A112000000001 SUBENT A1120001 19990319 0000A112000100001 BIB 11 31 A112000100002 INSTITUTE (1USALAS,1USACAL) A112000100003 REFERENCE (J,PR,104,(6),1639,195612) A112000100004 AUTHOR (L.CRANBERG,A.H.ARMSTRONG,R.L.HENKEL) A112000100005 TITLE Neutrons from the D-D reactions A112000100006 FACILITY (VDG,1USALAS) A112000100007 SAMPLE A gas target was 6 cm long, filled with D2 gas at a A112000100008 pressure of 60 cm of Hg, and sealed off from the A112000100009 vacuum system by a nickel foil 1.5mu thick. A112000100010 DETECTOR (SCIN) A112000100011 MONIT-REF (,CRANBERG+,J,PR,103,343,1956) A112000100012 MONITOR (1-H-3(P,N)2-HE-3,,DA) A112000100013 (1-H-2(D,N)2-HE-3,,DA) A112000100014 The two parts of the curve given by the two reactions A112000100015 were normalized to each other in the region several A112000100016 Mev wide in which they overlap. By means of the A112000100017 sensitivity curve obtained in this way,it is then A112000100018 possible to compare directly the yields obtained for A112000100019 the breakup neutrons and the neutrons from the reactionA112000100020 D(d,n)3He in terms of the known cross section of the A112000100021 latter reaction A112000100022 ERR-ANALYS (DATA-ERR) The errors are the sum of the statistical A112000100023 uncertainty and an additional error, which is hard A112000100024 to estimate, due to inaccuracy of the background A112000100025 subtraction. A112000100026 (DATA-ERR1) The uncertainty in the absolute value of A112000100027 the cross-section scale is due to the uncertainty of A112000100028 the normalizing procedure just referred to, and to the A112000100029 uncertainty in the cross section of the D(d,n)HE-3 A112000100030 reaction. A112000100031 HISTORY (19810525C) Compilation produced by Arzamas RFNC-VNIIEFA112000100032 (19990214U)CNPD: corrected 4-dig. year and lower cases.A112000100033 ENDBIB 31 0 A112000100034 COMMON 3 3 A112000100035 DATA-ERR1 EN-NRM ANG-NRM A112000100036 PER-CENT MEV ADEG A112000100037 5.0 10.5 0.0 A112000100038 ENDCOMMON 3 0 A112000100039 ENDSUBENT 38 0 A112000199999 SUBENT A1120002 19990319 0000A112000200001 BIB 2 2 A112000200002 REACTION (1-H-2(D,N+P)1-H-2,,DA,N,,EXP) A112000200003 STATUS (TABLE) Table 1 A112000200004 ENDBIB 2 0 A112000200005 COMMON 1 3 A112000200006 ANG A112000200007 ADEG A112000200008 0. A112000200009 ENDCOMMON 3 0 A112000200010 DATA 3 8 A112000200011 EN DATA DATA-ERR A112000200012 MEV MB/SR MB/SR A112000200013 4.75 0.24 0.06 A112000200014 5.28 1.5 0.02 A112000200015 5.78 5.4 0.3 A112000200016 6.21 11.4 0.6 A112000200017 6.31 12.9 0.6 A112000200018 6.8 19.8 1. A112000200019 7.16 30.2 2. A112000200020 7.33 32. 2. A112000200021 ENDDATA 10 0 A112000200022 ENDSUBENT 21 0 A112000299999 SUBENT A1120003 19990319 0000A112000300001 BIB 2 2 A112000300002 REACTION (1-H-2(D,N+P)1-H-2,,DA,N,,EXP) A112000300003 STATUS (TABLE) Table 2 A112000300004 ENDBIB 2 0 A112000300005 COMMON 1 3 A112000300006 EN A112000300007 MEV A112000300008 6.310 A112000300009 ENDCOMMON 3 0 A112000300010 DATA 3 5 A112000300011 ANG DATA DATA-ERR A112000300012 ADEG MB/SR MB/SR A112000300013 0. 13.5 0.7 A112000300014 10. 9. 0.5 A112000300015 20. 4.5 0.3 A112000300016 30. 2.8 0.2 A112000300017 40. 1.5 0.2 A112000300018 ENDDATA 7 0 A112000300019 ENDSUBENT 18 0 A112000399999 SUBENT A1120004 19990319 0000A112000400001 BIB 2 2 A112000400002 REACTION (1-H-2(D,N)2-HE-3,,DA,,,EXP) A112000400003 STATUS (TABLE) Table 2 A112000400004 ENDBIB 2 0 A112000400005 COMMON 1 3 A112000400006 EN A112000400007 MEV A112000400008 6.310 A112000400009 ENDCOMMON 3 0 A112000400010 DATA 3 5 A112000400011 ANG DATA DATA-ERR A112000400012 ADEG MB/SR MB/SR A112000400013 0. 80. 4. A112000400014 10. 56.9 3. A112000400015 20. 22.2 1. A112000400016 30. 5.5 0.4 A112000400017 40. 4.6 0.3 A112000400018 ENDDATA 7 0 A112000400019 ENDSUBENT 18 0 A112000499999 ENDENTRY 4 0 A112099999999