ENTRY D0016 20091113 D071D001600000001 SUBENT D0016001 20091113 D071D001600100001 BIB 9 16 D001600100002 INSTITUTE (1USABNW) D001600100003 REFERENCE (R,BNWL-1685,75,197211) D001600100004 AUTHOR (B.H.Duane) D001600100005 TITLE -The reaction rates for T(d,n)He-4, He-3(d,p)He-4, D001600100006 D(d,p)T, D(d,n)He-3, T(t,2n)He-4 and T(He3,x)Y.- D001600100007 FACILITY Unknown D001600100008 METHOD The reaction-rates were calculated, for the 6 reactionsD001600100009 the cross-sections are fitted by non-linear least D001600100010 squares. D001600100011 ERR-ANALYS no errors given. D001600100012 STATUS (TABLE)Data taken from table E.7 of BNWL-1685,p.75,1972D001600100013 HISTORY (19790424C) KO. D001600100014 (20011113A) updated to new date formats, lower case. D001600100015 (20060724A) SD. BIB upgrated. D001600100016 (20091113A) SD: value for 80 keV was corrected. D001600100017 1.023E-16 ==> 1.236E-16 D001600100018 ENDBIB 16 0 D001600100019 NOCOMMON 0 0 D001600100020 ENDSUBENT 19 0 D001600199999 SUBENT D0016002 20060725 D048D001600200001 BIB 3 19 D001600200002 REACTION (1-H-3(D,N)2-HE-4,,SGV,,,CALC) D001600200003 COMMENT the best theoretical representation of T(d,n)He-4 D001600200004 cross-sections which is fitted to the experiments is D001600200005 sig(E)= (a(2)/(1+(a(3)*E - a(4))**2)+a(5))/ D001600200006 (E(exp(a(1)/sqrt(E)) - 1)), D001600200007 where a(1) = 1453 +- 14 sqrt(eV) D001600200008 a(2) = (502 +- 26)**5 eV.barn D001600200009 a(3) = (1368 +- 45)**(-8)/eV D001600200010 a(4) = 1.076 +-.055 D001600200011 a(5) = (409 +- 15)**3 eV.barn. D001600200012 .the origin of the cross-section data is mentioned in D001600200013 'rel-ref'. D001600200014 REL-REF (R,C0018001,W.R.ARNOLD+,J,PR,93,483,1954) D001600200015 (R,C0008001,J.P.CONNER+,J,PR,88,468,1952) D001600200016 (R,C0001001,H.V.ARGO+,J,PR,87,612,1952) D001600200017 (R,,S.J.BAME+,J,BAP,1,93,1956) D001600200018 (R,A1352002,A.HEMMENDINGER+,J,PR,98,70,1955) D001600200019 (R,C0014002,T.F.STRATTON+,J,PR,88,261,1952) D001600200020 (R,C0038001,J.E.BROLLEY+,J,PR,82,502,1951) D001600200021 ENDBIB 19 0 D001600200022 NOCOMMON 0 0 D001600200023 DATA 2 24 D001600200024 KT DATA D001600200025 KEV CM3/SEC D001600200026 10.00 1.087E-16 D001600200027 19.00 3.937E-16 D001600200028 19.25 4.013E-16 D001600200029 19.33 4.039E-16 D001600200030 19.50 4.089E-16 D001600200031 19.75 4.165E-16 D001600200032 20.00 4.240E-16 D001600200033 30.00 6.649E-16 D001600200034 40.00 8.021E-16 D001600200035 50.00 8.701E-16 D001600200036 60.00 8.969E-16 D001600200037 70.00 8.999E-16 D001600200038 80.00 8.892E-16 D001600200039 90.00 8.708E-16 D001600200040 100.00 8.484E-16 D001600200041 200.00 6.276E-16 D001600200042 300.00 4.953E-16 D001600200043 400.00 4.168E-16 D001600200044 500.00 3.666E-16 D001600200045 600.00 3.327E-16 D001600200046 700.00 3.085E-16 D001600200047 800.00 2.908E-16 D001600200048 900.00 2.774E-16 D001600200049 1000.00 2.670E-16 D001600200050 ENDDATA 26 0 D001600200051 ENDSUBENT 50 0 D001600299999 SUBENT D0016003 20091113 D071D001600300001 BIB 4 21 D001600300002 REACTION (2-HE-3(D,P)2-HE-4,,SGV,,,CALC) D001600300003 COMMENT the best theoretical representation of He-3(d,p)He-4 D001600300004 cross-sections which is fitted to the experiment is D001600300005 sig(E)= (a(2)/(1+(a(3)*E - a(4))**2)+a(5))/ D001600300006 (E(exp(a(1)/sqrt(E)) - 1)), D001600300007 where a(1) = 2823 +- 35 sqrt(eV) D001600300008 a(2) = (259 +- 21)**5 eV-barn D001600300009 a(3) = (398 +- 13)**(-8) /eV D001600300010 a(4) = 1.297 +- .072 D001600300011 a(5) = (647 +- 41)**3 eV.barn D001600300012 .the origin of the cross-section data is mentioned in D001600300013 'rel-ref'. D001600300014 REL-REF (R,,R.G.JARVIS+,J,PRS/A,218,432,1953) D001600300015 (R,C0018001,W.R.ARNOLD+,J,PR,93,483,1954) D001600300016 (R,A1065001,W.E.KUNZ,J,PR,97,456,1955) D001600300017 (R,A1224001,G.FRIER+,J,PR,93,825,1954) D001600300018 (R,C0987002,J.L.YARNELL+,J,PR,90,292,1953) D001600300019 (R,A1064001,BONNER+,J,PR,88,473,1952) D001600300020 (R,A1091002,J.C.ALLRED,J,PR,84,695,1951) D001600300021 HISTORY (20091113A) SD: value for 80 keV was corrected. D001600300022 1.023E-16 ==> 1.236E-16 D001600300023 ENDBIB 21 0 D001600300024 NOCOMMON 0 0 D001600300025 DATA 2 24 D001600300026 KT DATA D001600300027 KEV CM3/SEC D001600300028 10.00 2.233E-19 D001600300029 19.00 3.140E-18 D001600300030 19.25 3.294E-18 D001600300031 19.33 3.347E-18 D001600300032 19.50 3.453E-18 D001600300033 19.75 3.617E-18 D001600300034 20.00 3.785E-18 D001600300035 30.00 1.451E-17 D001600300036 40.00 3.244E-17 D001600300037 50.00 5.435E-17 D001600300038 60.00 7.813E-17 D001600300039 70.00 1.016E-16 D001600300040 80.00 1.236E-16 D001600300041 90.00 1.435E-16 D001600300042 100.00 1.612E-16 D001600300043 200.00 2.432E-16 D001600300044 300.00 2.494E-16 D001600300045 400.00 2.386E-16 D001600300046 500.00 2.253E-16 D001600300047 600.00 2.130E-16 D001600300048 700.00 2.025E-16 D001600300049 800.00 1.936E-16 D001600300050 900.00 1.863E-16 D001600300051 1000.00 1.802E-16 D001600300052 ENDDATA 26 0 D001600300053 ENDSUBENT 52 0 D001600399999 SUBENT D0016004 20060725 D048D001600400001 BIB 3 15 D001600400002 REACTION (1-H-2(D,P)1-H-3,,SGV,,,CALC) D001600400003 COMMENT The best theoretical representation of D(d,p)T D001600400004 cross sections which is fitted to the experiments is D001600400005 sig(E)= (a(2)/(1+(a(3)*E - a(4))**2))/ D001600400006 (E(exp(a(1)/sqrt(E)) - 1)), D001600400007 where a(1) = 1457.7 +- 5.0 sqrt(eV) D001600400008 a(2) = (372 +- 10)**3 eV.barn D001600400009 a(3) = (436 +- 26)**(-9) /eV D001600400010 a(4) = 1.220 +- .038 D001600400011 .the origin of the cross-section data is mentioned in D001600400012 'rel-ref'. D001600400013 REL-REF (R,C0018001,W.R.ARNOLD+,J,PR,93,483,1954) D001600400014 (R,A1155001,W.A.WENZEL+,J,PR,88,1149,1952) D001600400015 (R,A1079001,J.M.BLAIR+,J,PR,74,1599,1948) D001600400016 (R,,G.PRESTON+,J,PRS/A,226,206,1954) D001600400017 ENDBIB 15 0 D001600400018 NOCOMMON 0 0 D001600400019 DATA 2 24 D001600400020 KT DATA D001600400021 KEV CM3/SEC D001600400022 10.00 5.809E-19 D001600400023 19.00 2.216E-18 D001600400024 19.25 2.270E-18 D001600400025 19.33 2.288E-18 D001600400026 19.50 2.323E-18 D001600400027 19.75 2.377E-18 D001600400028 20.00 2.432E-18 D001600400029 30.00 4.753E-18 D001600400030 40.00 7.200E-18 D001600400031 50.00 9.652E-18 D001600400032 60.00 1.206E-17 D001600400033 70.00 1.442E-17 D001600400034 80.00 1.672E-17 D001600400035 90.00 1.898E-17 D001600400036 100.00 2.118E-17 D001600400037 200.00 4.133E-17 D001600400038 300.00 5.845E-17 D001600400039 400.00 7.194E-17 D001600400040 500.00 8.173E-17 D001600400041 600.00 8.831E-17 D001600400042 700.00 9.237E-17 D001600400043 800.00 9.453E-17 D001600400044 900.00 9.530E-17 D001600400045 1000.00 9.508E-17 D001600400046 ENDDATA 26 0 D001600400047 ENDSUBENT 46 0 D001600499999 SUBENT D0016005 20060725 D048D001600500001 BIB 3 18 D001600500002 REACTION (1-H-2(D,N)2-HE-3,,SGV,,,CALC) D001600500003 COMMENT The best theoretical representation of D(d,n)He-3 D001600500004 cross sections which is fitted to the experiments is D001600500005 sig(E)= (a(2)/(1+(a(3)*E - a(4))**2))/ D001600500006 (E(exp(a(1)/sqrt(E)) - 1)), D001600500007 where a(1) = 1514 +- 13 sqrt(eV) D001600500008 a(2) = (482 +- 29)**3 eV-barn D001600500009 a(3) = (308 +- 37)**(-9) /eV D001600500010 a(4) = 1.177 +- .077 D001600500011 .the origin of the cross-section data is mentioned in D001600500012 'rel-ref'. D001600500013 REL-REF (R,C0018001,W.R.ARNOLD+,J,PR,93,483,1954) D001600500014 (R,,R.K.SMITH+,W,SMITH,1957) quoted in Liskien,Paulsen D001600500015 nucl.data table,11(1973)569. D001600500016 (R,A1150001,G.T.HUNTER+,J,PR,76,1445,1949) D001600500017 (R,A1079001,J.M.BLAIR+,J,PR,74,1599,1948) D001600500018 (R,,G.PRESTON+,J,PRS/A,226,206,1954) D001600500019 (R,A1070001,K.W.ERICKSON+,J,PR,76,1141,1949) D001600500020 ENDBIB 18 0 D001600500021 NOCOMMON 0 0 D001600500022 DATA 2 24 D001600500023 KT DATA D001600500024 KEV CM3/SEC D001600500025 10.00 6.259E-19 D001600500026 19.00 2.478E-18 D001600500027 19.25 2.539E-18 D001600500028 19.33 2.559E-18 D001600500029 19.50 2.601E-18 D001600500030 19.75 2.663E-18 D001600500031 20.00 2.725E-18 D001600500032 30.00 5.410E-18 D001600500033 40.00 8.259E-18 D001600500034 50.00 1.111E-17 D001600500035 60.00 1.391E-17 D001600500036 70.00 1.663E-17 D001600500037 80.00 1.927E-17 D001600500038 90.00 2.182E-17 D001600500039 100.00 2.431E-17 D001600500040 200.00 4.624E-17 D001600500041 300.00 6.500E-17 D001600500042 400.00 8.117E-17 D001600500043 500.00 9.465E-17 D001600500044 600.00 1.054E-16 D001600500045 700.00 1.136E-16 D001600500046 800.00 1.196E-16 D001600500047 900.00 1.239E-16 D001600500048 1000.00 1.266E-16 D001600500049 ENDDATA 26 0 D001600500050 ENDSUBENT 49 0 D001600599999 SUBENT D0016006 20060725 D048D001600600001 BIB 3 12 D001600600002 REACTION (1-H-3(T,2N)2-HE-4,,SGV,,,CALC) D001600600003 COMMENT the best theoretical presentation of t(t,2n)he-4 D001600600004 cross sections which is fitted to the experiment is D001600600005 sig(E)= (a(2)/(1+(a(3)*E - a(4))**2))/ D001600600006 (E(exp(a(1)/sqrt(E))-1)) , D001600600007 where a(1) = 1214 +- 72 sqrt(eV) D001600600008 a(2) = (448 +- 59)**3 eV-barn D001600600009 a(3) = (102 +- 10)**(-8) /eV D001600600010 a(4) = 2.09 +- 0.14 D001600600011 .the origin of the cross-section data is mentioned in D001600600012 'rel-ref'. D001600600013 REL-REF (R,A1089001,H.M.AGNEW+,J,PR,84,862,1951) D001600600014 ENDBIB 12 0 D001600600015 NOCOMMON 0 0 D001600600016 DATA 2 24 D001600600017 KT DATA D001600600018 KEV CM3/SEC D001600600019 10.00 7.243E-19 D001600600020 19.00 2.322E-18 D001600600021 19.25 2.371E-18 D001600600022 19.33 2.387E-18 D001600600023 19.50 2.420E-18 D001600600024 19.75 2.469E-18 D001600600025 20.00 2.519E-18 D001600600026 30.00 4.554E-18 D001600600027 40.00 6.624E-18 D001600600028 50.00 8.686E-18 D001600600029 60.00 1.074E-17 D001600600030 70.00 1.280E-17 D001600600031 80.00 1.489E-17 D001600600032 90.00 1.701E-17 D001600600033 100.00 1.918E-17 D001600600034 200.00 4.267E-17 D001600600035 300.00 6.337E-17 D001600600036 400.00 7.679E-17 D001600600037 500.00 8.384E-17 D001600600038 600.00 8.655E-17 D001600600039 700.00 8.654E-17 D001600600040 800.00 8.494E-17 D001600600041 900.00 8.242E-17 D001600600042 1000.00 7.943E-17 D001600600043 ENDDATA 26 0 D001600600044 ENDSUBENT 43 0 D001600699999 SUBENT D0016007 20060725 D048D001600700001 BIB 4 29 D001600700002 REACTION ((2-HE-3(T,N+P)2-HE-4,,SGV,,,CALC)+ D001600700003 (2-HE-3(T,D)2-HE-4,,SGV,,,CALC)+ D001600700004 (2-HE-3(T,P)2-HE-5,,SGV,,,CALC)) D001600700005 COMMENT The best theoretical presentation of T(He3,x)Y D001600700006 cross sections which is fitted to the experiment is D001600700007 sig(E)= (a(2))/(E(exp(a(1)/sqrt(E))-1)) , D001600700008 where a(1) = 3893 +- 34 sqrt(eV) D001600700009 a(2) = (1125 +- 68)**4 eV-barn. D001600700010 probability (225 to 600 keV) x y D001600700011 --------------------------------------------------- D001600700012 .51 +- .02 p + n He-4 D001600700013 .43 +- .02 d He-4 D001600700014 .06 +- .02 p He-5 D001600700015 --------------------------------------------------- D001600700016 the origin of the cross-section data is mentioned in D001600700017 'rel-ref'. D001600700018 ===compiler's note (cited from Phys.Rev.,92(1953)383) D001600700019 when 3H is bombarded by 3He, D001600700020 3H + 3He to 6*Li and to 4He + 2H + 14.31 MeV, D001600700021 to 4He + 1H + n + 12.08 MeV, D001600700022 and to 5*He + 1H + Q-value. D001600700023 The Q-value of the last reaction depends upon the D001600700024 excitation energy left in the 5He nucleus. if 5He D001600700025 is left in its ground state, Q will be equal to D001600700026 12.08-E(5He), where E(5He) is the energy of breakup ofD001600700027 5He into neutron and an alpha particle. === D001600700028 REL-REF (R,A1227001,C.D.MOAK,J,PR,92,383,195310) D001600700029 HISTORY (20011113A) leading parenthesis added to reaction; D001600700030 first reaction sequence corrected. D001600700031 ENDBIB 29 0 D001600700032 NOCOMMON 0 0 D001600700033 DATA 2 24 D001600700034 KT DATA D001600700035 KEV CM3/SEC D001600700036 10.00 1.156E-20 D001600700037 19.00 2.142E-19 D001600700038 19.25 2.256E-19 D001600700039 19.33 2.295E-19 D001600700040 19.50 2.374E-19 D001600700041 19.75 2.496E-19 D001600700042 20.00 2.623E-19 D001600700043 30.00 1.134E-18 D001600700044 40.00 2.805E-18 D001600700045 50.00 5.287E-18 D001600700046 60.00 8.515E-18 D001600700047 70.00 1.240E-17 D001600700048 80.00 1.685E-17 D001600700049 90.00 2.178E-17 D001600700050 100.00 2.712E-17 D001600700051 200.00 9.177E-17 D001600700052 300.00 1.606E-16 D001600700053 400.00 2.256E-16 D001600700054 500.00 2.852E-16 D001600700055 600.00 3.397E-16 D001600700056 700.00 3.895E-16 D001600700057 800.00 4.352E-16 D001600700058 900.00 4.772E-16 D001600700059 1000.00 5.161E-16 D001600700060 ENDDATA 26 0 D001600700061 ENDSUBENT 60 0 D001600799999 ENDENTRY 7 0 D001699999999