ENTRY F0126 20200508 F077F012600000001 SUBENT F0126001 20200508 F077F012600100001 BIB 10 17 F012600100002 TITLE Study of the reactions T(p,n)3He,7Li(p,n)7Be, F012600100003 9Be(p,n)9B and 19F(p,n)19Ne F012600100004 AUTHOR (J.B.Marion,T.W.Bonner,C.F.Cook) F012600100005 INSTITUTE (1USARIC) F012600100006 REFERENCE (J,PR,100,91,1955) F012600100007 FACILITY (VDG,1USARIC) F012600100008 METHOD Counter ratio technique was used (see REL-REF). F012600100009 REL-REF (M,,J.B.Marion+,J,PR,100,46,1955) - Counter ratio F012600100010 technique description. F012600100011 DETECTOR (LONGC) F012600100012 ADD-RES Data for reactions T(p,n)3He and 7Li(p,n)7Be are givenF012600100013 in counter ratio units. F012600100014 HISTORY (19800922C) F012600100015 (19990409U) CNPD: corrected 4-dig. year and lower casesF012600100016 (20200508A) SD: Corrections in all Subents. Subents F012600100017 004-007 added. SAMPLE moved to Subents 002-005. F012600100018 BIB updated. F012600100019 ENDBIB 17 0 F012600100020 NOCOMMON 0 0 F012600100021 ENDSUBENT 20 0 F012600199999 SUBENT F0126002 20200508 F077F012600200001 BIB 5 14 F012600200002 REACTION (4-BE-9(P,N)5-B-9,,DA) F012600200003 SAMPLE An evaporated beryllium target, about 8 keV thick at a F012600200004 proton energy of 2 MeV, was used in the experiment. F012600200005 The counter ratio and the yield of neutrons in the F012600200006 forward direction were measured for proton energies F012600200007 from threshold to 5.8 MeV. F012600200008 ANALYSIS A study was done with the counter ratio technique the F012600200009 low-lying level structure of the residual nuclei. F012600200010 STATUS (CURVE) Fig 4 Phys.Rev.,100(1955)91 F012600200011 (DEP,F0126004) Value used for normalization. F012600200012 HISTORY (20200507A) SD: SF9=EXP deleted from REACTION code. F012600200013 EN-ERR -> EN-ERR-DIG; DATA-ERR -> ERR-DIG. ERR-ANALYS F012600200014 deleted. STATUS updated. FLAG deleted (Value moved to F012600200015 Subent 004). F012600200016 ENDBIB 14 0 F012600200017 COMMON 4 3 F012600200018 ANG-MIN ANG-MAX EN-ERR-DIG ERR-DIG F012600200019 ADEG ADEG MEV MB/SR F012600200020 0.0 10. 0.04 0.5 F012600200021 ENDCOMMON 3 0 F012600200022 DATA 2 109 F012600200023 EN DATA F012600200024 MEV MB/SR F012600200025 1.88 0.1 F012600200026 1.90 0.8 F012600200027 1.90 0.3 F012600200028 1.91 0.1 F012600200029 1.92 0.0 F012600200030 1.94 0.7 F012600200031 1.94 0.3 F012600200032 1.95 0.7 F012600200033 1.95 1.1 F012600200034 1.97 0.5 F012600200035 2.02 0.6 F012600200036 2.06 0.8 F012600200037 2.11 1.3 F012600200038 2.15 1.5 F012600200039 2.18 1.8 F012600200040 2.23 2.2 F012600200041 2.26 2.7 F012600200042 2.31 3.1 F012600200043 2.38 4.5 F012600200044 2.42 5.5 F012600200045 2.45 6.7 F012600200046 2.46 7.7 F012600200047 2.48 8.5 F012600200048 2.49 8.9 F012600200049 2.51 9.6 F012600200050 2.52 10.4 F012600200051 2.55 11.4 F012600200052 2.57 12.1 F012600200053 2.58 12.6 F012600200054 2.61 11.6 F012600200055 2.62 9.9 F012600200056 2.63 8.6 F012600200057 2.67 7.9 F012600200058 2.71 7.5 F012600200059 2.76 7.6 F012600200060 2.80 7.6 F012600200061 2.83 7.6 F012600200062 2.87 7.7 F012600200063 2.95 7.9 F012600200064 2.98 7.9 F012600200065 3.03 8.1 F012600200066 3.08 8.4 F012600200067 3.16 8.7 F012600200068 3.23 9.2 F012600200069 3.31 9.7 F012600200070 3.40 10.5 F012600200071 3.48 11.3 F012600200072 3.56 12.0 F012600200073 3.63 12.7 F012600200074 3.71 13.5 F012600200075 3.79 14.3 F012600200076 3.80 14.7 F012600200077 3.82 15.0 F012600200078 3.88 15.9 F012600200079 3.92 16.4 F012600200080 3.96 17.4 F012600200081 4.01 18.4 F012600200082 4.03 19.1 F012600200083 4.07 19.8 F012600200084 4.11 21.1 F012600200085 4.13 21.6 F012600200086 4.15 22.3 F012600200087 4.21 24.3 F012600200088 4.27 26.0 F012600200089 4.28 26.5 F012600200090 4.35 28.8 F012600200091 4.40 30.2 F012600200092 4.44 32.2 F012600200093 4.47 33.4 F012600200094 4.48 34.1 F012600200095 4.52 35.7 F012600200096 4.53 36.6 F012600200097 4.56 37.6 F012600200098 4.58 39.1 F012600200099 4.60 40.0 F012600200100 4.62 40.7 F012600200101 4.63 41.3 F012600200102 4.65 42.3 F012600200103 4.70 43.1 F012600200104 4.71 43.1 F012600200105 4.73 43.0 F012600200106 4.77 42.2 F012600200107 4.79 41.7 F012600200108 4.81 41.2 F012600200109 4.84 40.7 F012600200110 4.87 40.6 F012600200111 4.90 40.4 F012600200112 4.93 40.2 F012600200113 4.96 39.3 F012600200114 4.97 39.0 F012600200115 4.99 38.4 F012600200116 5.01 37.6 F012600200117 5.05 36.5 F012600200118 5.09 36.5 F012600200119 5.13 36.2 F012600200120 5.19 36.2 F012600200121 5.21 36.0 F012600200122 5.26 35.9 F012600200123 5.30 35.6 F012600200124 5.33 35.6 F012600200125 5.37 35.7 F012600200126 5.42 36.0 F012600200127 5.45 36.2 F012600200128 5.50 36.6 F012600200129 5.54 36.6 F012600200130 5.58 36.9 F012600200131 5.63 37.1 F012600200132 5.67 37.1 F012600200133 5.70 37.6 F012600200134 ENDDATA 111 0 F012600200135 ENDSUBENT 134 0 F012600299999 SUBENT F0126003 20200508 F077F012600300001 BIB 5 13 F012600300002 REACTION (9-F-19(P,N)10-NE-19,,DA) F012600300003 SAMPLE An evaporated A1F3 target, which was about 7 keV thick F012600300004 at a proton energy of 4.5 MeV, was used in the F012600300005 experiment. The counter ratio and the forward yield of F012600300006 neutrons were measured from threshold to 5.9 MeV. F012600300007 ANALYSIS A study was done with the counter ratio technique the F012600300008 low-lying level structure of the residual nuclei. F012600300009 STATUS (CURVE) Fig 5 Phys.Rev.,100(1955)91 F012600300010 (DEP,F0126005) Value used for normalization. F012600300011 HISTORY (20200507A) SD: SF9=EXP deleted from REACTION code. F012600300012 EN-ERR -> EN-ERR-DIG; DATA-ERR -> ERR-DIG. ERR-ANALYS F012600300013 deleted. STATUS updated. FLAG deleted (Value moved to F012600300014 Subent 005). F012600300015 ENDBIB 13 0 F012600300016 COMMON 4 3 F012600300017 ANG-MIN ANG-MAX EN-ERR-DIG ERR-DIG F012600300018 ADEG ADEG MEV MB/SR F012600300019 0.0 10. 0.01 0.07 F012600300020 ENDCOMMON 3 0 F012600300021 DATA 2 70 F012600300022 EN DATA F012600300023 MEV MB/SR F012600300024 4.23 0.26 F012600300025 4.25 0.26 F012600300026 4.27 0.48 F012600300027 4.28 0.66 F012600300028 4.30 0.96 F012600300029 4.33 1.27 F012600300030 4.35 1.66 F012600300031 4.36 1.83 F012600300032 4.37 2.05 F012600300033 4.39 2.58 F012600300034 4.40 2.92 F012600300035 4.40 3.23 F012600300036 4.41 3.88 F012600300037 4.42 4.32 F012600300038 4.43 4.93 F012600300039 4.45 5.54 F012600300040 4.45 5.80 F012600300041 4.46 6.28 F012600300042 4.47 6.63 F012600300043 4.49 6.89 F012600300044 4.50 6.80 F012600300045 4.51 6.63 F012600300046 4.52 7.02 F012600300047 4.52 7.33 F012600300048 4.54 7.54 F012600300049 4.54 7.80 F012600300050 4.55 8.15 F012600300051 4.56 8.28 F012600300052 4.58 8.89 F012600300053 4.59 9.59 F012600300054 4.61 10.20 F012600300055 4.62 10.59 F012600300056 4.64 11.38 F012600300057 4.65 11.38 F012600300058 4.67 11.12 F012600300059 4.68 11.16 F012600300060 4.70 11.29 F012600300061 4.71 11.86 F012600300062 4.75 13.25 F012600300063 4.79 15.56 F012600300064 4.82 14.69 F012600300065 4.83 13.30 F012600300066 4.86 11.26 F012600300067 4.88 10.21 F012600300068 4.92 9.08 F012600300069 4.96 7.96 F012600300070 4.98 8.13 F012600300071 5.00 10.09 F012600300072 5.04 9.00 F012600300073 5.09 10.31 F012600300074 5.13 10.66 F012600300075 5.17 12.84 F012600300076 5.21 15.15 F012600300077 5.26 19.63 F012600300078 5.30 20.50 F012600300079 5.34 19.98 F012600300080 5.38 18.20 F012600300081 5.42 18.07 F012600300082 5.46 16.55 F012600300083 5.51 15.16 F012600300084 5.55 14.77 F012600300085 5.59 14.51 F012600300086 5.63 15.04 F012600300087 5.68 19.91 F012600300088 5.71 22.35 F012600300089 5.75 23.09 F012600300090 5.78 22.40 F012600300091 5.80 19.61 F012600300092 5.85 14.09 F012600300093 5.89 18.14 F012600300094 ENDDATA 72 0 F012600300095 ENDSUBENT 94 0 F012600399999 SUBENT F0126004 20200508 F077F012600400001 BIB 7 12 F012600400002 REACTION (4-BE-9(P,N)5-B-9,,DA) F012600400003 SAMPLE A 9Be target of 171 mu-g/cm2 F012600400004 MONITOR (3-LI-7(P,N)4-BE-7,,SIG) F012600400005 MONIT-REF (F0023001,R.Taschek+,J,PR,74,373,1948) F012600400006 ANALYSIS The cross sections were determined by comparing F012600400007 the counting rates in a long counter from the proton F012600400008 bombardment of these targets with that from a weighted F012600400009 LiF target, since the cross section for the reaction F012600400010 7Li(p,n) is well known. F012600400011 STATUS (TABLE) Value from the text on p.96 of F012600400012 Phys.Rev.,100(1955)91 F012600400013 HISTORY (20200507T) SD: Value from Subent 002. F012600400014 ENDBIB 12 0 F012600400015 NOCOMMON 0 0 F012600400016 DATA 4 1 F012600400017 EN ANG-MIN ANG-MAX DATA F012600400018 MEV ADEG ADEG MB/SR F012600400019 2.52 0.0 10. 11. F012600400020 ENDDATA 3 0 F012600400021 ENDSUBENT 20 0 F012600499999 SUBENT F0126005 20200508 F077F012600500001 BIB 7 12 F012600500002 REACTION (9-F-19(P,N)10-NE-19,,DA) F012600500003 SAMPLE An evaporated AlF3 target about 447 mu-g/cm2. F012600500004 MONITOR (3-LI-7(P,N)4-BE-7,,SIG) F012600500005 MONIT-REF (F0023001,R.Taschek+,J,PR,74,373,1948) F012600500006 ANALYSIS The cross sections were determined by comparing F012600500007 the counting rates in a long counter from the proton F012600500008 bombardment of these targets with that from a weighted F012600500009 LiF target, since the cross section for the reaction F012600500010 7Li(p,n) is well known. F012600500011 STATUS (TABLE) Value from the text on p.96 of F012600500012 Phys.Rev.,100(1955)91 F012600500013 HISTORY (20200507T) SD: Value from Subent 003. F012600500014 ENDBIB 12 0 F012600500015 NOCOMMON 0 0 F012600500016 DATA 4 1 F012600500017 EN ANG-MIN ANG-MAX DATA F012600500018 MEV ADEG ADEG MB/SR F012600500019 4.74 0.0 10. 13. F012600500020 ENDDATA 3 0 F012600500021 ENDSUBENT 20 0 F012600599999 SUBENT F0126006 20200508 F077F012600600001 BIB 8 13 F012600600002 REACTION (5-B-11(P,N)6-C-11,,DA) F012600600003 SAMPLE A 11B target of 46 mu-g/cm2 F012600600004 MONITOR (3-LI-7(P,N)4-BE-7,,SIG) F012600600005 MONIT-REF (F0023001,R.Taschek+,J,PR,74,373,1948) F012600600006 REL-REF (A,F0322001,J.K.Bair+,J,PR,100,21,1955) F012600600007 (A,D0095002,J.P.Blaser+,J,HPA,24,465,1951) F012600600008 ANALYSIS The cross sections were determined by comparing F012600600009 the counting rates in a long counter from the proton F012600600010 bombardment of these targets with that from a weighted F012600600011 LiF target, since the cross section for the reaction F012600600012 7Li(p,n) is well known. F012600600013 STATUS (TABLE) Tbl. III from Phys.Rev.,100(1955)91 F012600600014 HISTORY (20200507C) SD F012600600015 ENDBIB 13 0 F012600600016 NOCOMMON 0 0 F012600600017 DATA 4 1 F012600600018 EN ANG-MIN ANG-MAX DATA F012600600019 MEV ADEG ADEG MB/SR F012600600020 3.46 0.0 10. 15. F012600600021 ENDDATA 3 0 F012600600022 ENDSUBENT 21 0 F012600699999 SUBENT F0126007 20200508 F077F012600700001 BIB 8 13 F012600700002 REACTION (6-C-13(P,N)7-N-13,,DA) F012600700003 SAMPLE A 13C target of 190 mu-g/cm2 F012600700004 MONITOR (3-LI-7(P,N)4-BE-7,,SIG) F012600700005 MONIT-REF (F0023001,R.Taschek+,J,PR,74,373,1948) F012600700006 REL-REF (A,,J.K.Bair+,J,PR,90,575,1953) F012600700007 (A,D0095002,J.P.Blaser+,J,HPA,24,465,1951) F012600700008 ANALYSIS The cross sections were determined by comparing F012600700009 the counting rates in a long counter from the proton F012600700010 bombardment of these targets with that from a weighted F012600700011 LiF target, since the cross section for the reaction F012600700012 7Li(p,n) is well known. F012600700013 STATUS (TABLE) Tbl. III from Phys.Rev.,100(1955)91 F012600700014 HISTORY (20200507C) SD F012600700015 ENDBIB 13 0 F012600700016 NOCOMMON 0 0 F012600700017 DATA 4 1 F012600700018 EN ANG-MIN ANG-MAX DATA F012600700019 MEV ADEG ADEG MB/SR F012600700020 3.70 0.0 10. 6.7 F012600700021 ENDDATA 3 0 F012600700022 ENDSUBENT 21 0 F012600799999 ENDENTRY 7 0 F012699999999