ENTRY A1159 20210125 A096A115900000001 SUBENT A1159001 20210125 A096A115900100001 BIB 7 15 A115900100002 TITLE Differential cross sections for the T(p,n)3He reaction A115900100003 AUTHOR (W.E.Wilson,R.L.Walter,D.B.Fossan) A115900100004 REFERENCE (J,NP,27,421,1961) - final data of T(p,n)3He reaction A115900100005 (J,BAP,5,410(D9),1960) - prelim.data of T(p,n); A115900100006 T(p,n+p) and D(d,n+p) reactions A115900100007 (T,WILSON,1961) 'Neutrons from p+T and D+D', A115900100008 W.E.Wilson, Theses, University of Wisconsin A115900100009 - full description of the experiment A115900100010 INSTITUTE (1USAWIS) A115900100011 FACILITY (VDGT,1USAWIS) A115900100012 METHOD (PHD,EDE) A115900100013 HISTORY (19820817C) Compilation produced by Arzamas RFNC-VNIIEFA115900100014 (19990220U)CNPD: corrected 4-dig. year and lower cases.A115900100015 (20210125A) SD: Corrections in all Subents. BIB updatedA115900100016 Subents 005-007 added. A115900100017 ENDBIB 15 0 A115900100018 NOCOMMON 0 0 A115900100019 ENDSUBENT 18 0 A115900199999 SUBENT A1159002 20210125 A096A115900200001 BIB 7 19 A115900200002 REACTION (1-H-3(P,N)2-HE-3,,DA) A115900200003 SAMPLE The tritium gas was contained in a thin-walled steel A115900200004 cylinder 2 cm long and 0.6 cm in diam. Target A115900200005 pressures were such that the tritium gas caused 5 and A115900200006 13 MeV protons to lose 40 and 30 keV of energy, A115900200007 respectively. A115900200008 DETECTOR (SCIN) The stilbene crystal was 0.6 cm thick and A115900200009 and 25 mm in diameter, mounted on an RCA6342A A115900200010 photomultiplier tube, was used as the detector. A115900200011 The angle subtended by the crystal at the A115900200012 target was about 4.5 degr. A115900200013 MONITOR (1-H-3(P,N)2-HE-3,,DA) A115900200014 ERR-ANALYS (ERR-T) Total error A115900200015 (ERR-S,1.5,5.) statistical error A115900200016 STATUS (CURVE) Figs 4,5 from Nucl.Phys.,27(1961)421 A115900200017 (same figs 9,10 in Wilson's thesis) A115900200018 (DEP,A1159007) Monitor cr.section A115900200019 HISTORY (20210125A) SD: SF9=EXP deleted from A115900200020 REACTION code. Data re-digitized. BIB updated. A115900200021 ENDBIB 19 0 A115900200022 COMMON 4 3 A115900200023 ANG-NRM ERR-T COS-ERR-D ERR-DIG A115900200024 ADEG PER-CENT NO-DIM MB/SR A115900200025 0. 15.0 0.0033 0.35 A115900200026 ENDCOMMON 3 0 A115900200027 DATA 3 265 A115900200028 EN COS-CM DATA-CM A115900200029 MEV NO-DIM MB/SR A115900200030 4.94 -0.9426 87.89 A115900200031 4.94 -0.9001 83.68 A115900200032 4.94 -0.8360 68.99 A115900200033 4.94 -0.7539 57.78 A115900200034 4.94 -0.6485 45.14 A115900200035 4.94 -0.5252 33.52 A115900200036 4.94 -0.3770 23.95 A115900200037 4.94 -0.2027 16.73 A115900200038 4.94 -0.0089 14.12 A115900200039 4.94 0.1890 14.09 A115900200040 4.94 0.3912 17.13 A115900200041 4.94 0.5825 21.61 A115900200042 4.94 0.7490 27.02 A115900200043 4.94 0.8784 32.12 A115900200044 4.94 0.9665 35.70 A115900200045 4.94 0.9940 36.82 A115900200046 5.44 -0.9434 84.18 A115900200047 5.44 -0.8956 75.86 A115900200048 5.44 -0.8341 65.48 A115900200049 5.44 -0.7506 53.05 A115900200050 5.44 -0.6465 41.33 A115900200051 5.44 -0.5191 28.47 A115900200052 5.44 -0.3682 19.31 A115900200053 5.44 -0.1979 14.35 A115900200054 5.44 -0.0111 12.06 A115900200055 5.44 0.1966 12.84 A115900200056 5.44 0.3932 16.09 A115900200057 5.44 0.5858 19.75 A115900200058 5.44 0.7509 22.79 A115900200059 5.44 0.8803 26.87 A115900200060 5.44 0.9959 30.34 A115900200061 5.94 -0.9429 79.14 A115900200062 5.94 -0.8937 70.51 A115900200063 5.94 -0.8308 59.41 A115900200064 5.94 -0.7488 45.85 A115900200065 5.94 -0.6434 34.02 A115900200066 5.94 -0.5186 23.94 A115900200067 5.94 -0.3649 16.83 A115900200068 5.94 -0.1904 12.38 A115900200069 5.94 0.0020 12.25 A115900200070 5.94 0.1986 13.85 A115900200071 5.94 0.4035 15.35 A115900200072 5.94 0.5865 18.50 A115900200073 5.94 0.7570 20.52 A115900200074 5.94 0.8822 23.06 A115900200075 5.94 0.9703 25.41 A115900200076 5.94 0.9978 25.40 A115900200077 6.44 -0.9396 73.07 A115900200078 6.44 -0.8931 65.77 A115900200079 6.44 -0.8276 54.47 A115900200080 6.44 -0.7455 40.80 A115900200081 6.44 -0.6401 29.60 A115900200082 6.44 -0.5139 19.72 A115900200083 6.44 -0.3629 14.66 A115900200084 6.44 -0.1912 11.34 A115900200085 6.44 -0.0015 10.90 A115900200086 6.44 0.2034 12.40 A115900200087 6.44 0.4042 14.72 A115900200088 6.44 0.5898 16.43 A115900200089 6.44 0.7576 17.84 A115900200090 6.44 0.8841 19.45 A115900200091 6.44 0.9667 21.29 A115900200092 6.44 0.9942 21.79 A115900200093 6.94 -0.9419 72.57 A115900200094 6.94 -0.8971 62.50 A115900200095 6.94 -0.8291 49.85 A115900200096 6.94 -0.7458 38.13 A115900200097 6.94 -0.6420 26.50 A115900200098 6.94 -0.5146 18.04 A115900200099 6.94 -0.3650 12.45 A115900200100 6.94 -0.1905 11.06 A115900200101 6.94 0.0020 11.21 A115900200102 6.94 0.2014 13.10 A115900200103 6.94 0.4008 14.58 A115900200104 6.94 0.5892 15.25 A115900200105 6.94 0.7542 16.12 A115900200106 6.94 0.8835 16.90 A115900200107 6.94 0.9633 18.01 A115900200108 6.94 0.9935 18.51 A115900200109 7.43 -0.9460 68.76 A115900200110 7.43 -0.8957 57.76 A115900200111 7.43 -0.8289 46.65 A115900200112 7.43 -0.7471 34.93 A115900200113 7.43 -0.6404 24.73 A115900200114 7.43 -0.5157 16.38 A115900200115 7.43 -0.3620 11.61 A115900200116 7.43 -0.1902 10.74 A115900200117 7.43 -0.0005 11.61 A115900200118 7.43 0.2003 13.19 A115900200119 7.43 0.4011 14.77 A115900200120 7.43 0.5908 15.23 A115900200121 7.43 0.7558 15.18 A115900200122 7.43 0.8837 16.07 A115900200123 7.43 0.9676 16.86 A115900200124 7.43 0.9965 17.06 A115900200125 7.93 -0.9430 67.00 A115900200126 7.93 -0.8928 54.97 A115900200127 7.93 -0.8274 44.58 A115900200128 7.93 -0.7469 32.24 A115900200129 7.93 -0.6416 21.64 A115900200130 7.93 -0.5155 14.72 A115900200131 7.93 -0.3617 11.29 A115900200132 7.93 -0.1872 10.72 A115900200133 7.93 -0.0001 12.31 A115900200134 7.93 0.2006 13.48 A115900200135 7.93 0.4041 13.42 A115900200136 7.93 0.5924 13.26 A115900200137 7.93 0.7601 13.42 A115900200138 7.93 0.8825 13.58 A115900200139 7.93 0.9706 14.99 A115900200140 7.93 1.0008 15.29 A115900200141 8.45 -0.9460 57.74 A115900200142 8.45 -0.8983 49.72 A115900200143 8.45 -0.8302 38.20 A115900200144 8.45 -0.7455 27.19 A115900200145 8.45 -0.6401 18.85 A115900200146 8.45 -0.5084 12.96 A115900200147 8.45 -0.3615 10.86 A115900200148 8.45 -0.1827 10.91 A115900200149 8.45 0.0015 12.39 A115900200150 8.45 0.2037 13.15 A115900200151 8.45 0.4044 13.09 A115900200152 8.45 0.5913 12.83 A115900200153 8.45 0.7604 13.09 A115900200154 8.45 0.8856 13.57 A115900200155 8.45 0.9695 14.77 A115900200156 8.45 0.9970 14.97 A115900200157 8.93 -0.9490 53.93 A115900200158 8.93 -0.8955 45.26 A115900200159 8.93 -0.8310 34.42 A115900200160 8.93 -0.7475 24.52 A115900200161 8.93 -0.6395 16.38 A115900200162 8.93 -0.5125 11.55 A115900200163 8.93 -0.3489 10.04 A115900200164 8.93 -0.1895 10.18 A115900200165 8.93 0.0012 11.88 A115900200166 8.93 0.2001 12.65 A115900200167 8.93 0.3977 12.49 A115900200168 8.93 0.5872 12.02 A115900200169 8.93 0.7480 11.54 A115900200170 8.93 0.8747 12.70 A115900200171 8.93 0.9591 14.27 A115900200172 8.93 0.9905 14.38 A115900200173 9.42 -0.9451 46.23 A115900200174 9.42 -0.8958 39.73 A115900200175 9.42 -0.8273 31.48 A115900200176 9.42 -0.7411 21.88 A115900200177 9.42 -0.6331 14.88 A115900200178 9.42 -0.5090 10.36 A115900200179 9.42 -0.3577 10.29 A115900200180 9.42 -0.1846 10.33 A115900200181 9.42 0.0061 12.55 A115900200182 9.42 0.2037 12.39 A115900200183 9.42 0.4040 11.82 A115900200184 9.42 0.5894 11.55 A115900200185 9.42 0.7515 11.69 A115900200186 9.42 0.8783 11.93 A115900200187 9.42 0.9599 14.12 A115900200188 9.42 0.9899 14.44 A115900200189 9.92 -0.9453 47.00 A115900200190 9.92 -0.8949 39.80 A115900200191 9.92 -0.8280 30.43 A115900200192 9.92 -0.7435 22.92 A115900200193 9.92 -0.6385 14.69 A115900200194 9.92 -0.5077 11.09 A115900200195 9.92 -0.3578 10.89 A115900200196 9.92 -0.1847 11.82 A115900200197 9.92 0.0020 13.17 A115900200198 9.92 0.2010 13.38 A115900200199 9.92 0.3986 12.46 A115900200200 9.92 0.5880 11.64 A115900200201 9.92 0.7515 11.65 A115900200202 9.92 0.8769 12.17 A115900200203 9.92 0.9900 15.16 A115900200204 10.42 -0.9438 34.06 A115900200205 10.42 -0.8933 28.91 A115900200206 10.42 -0.8292 22.84 A115900200207 10.42 -0.7433 16.87 A115900200208 10.42 -0.6370 11.21 A115900200209 10.42 -0.5048 9.36 A115900200210 10.42 -0.3576 9.58 A115900200211 10.42 -0.1818 10.92 A115900200212 10.42 0.0076 12.47 A115900200213 10.42 0.2066 12.69 A115900200214 10.42 0.4042 11.66 A115900200215 10.42 0.5936 10.85 A115900200216 10.42 0.7530 10.85 A115900200217 10.42 0.8825 11.68 A115900200218 10.42 0.9642 14.67 A115900200219 10.42 0.9929 15.50 A115900200220 11.09 -0.5046 8.57 A115900200221 11.09 -0.3507 8.78 A115900200222 11.09 -0.1789 10.02 A115900200223 11.09 0.0091 11.68 A115900200224 11.09 0.2081 11.89 A115900200225 11.09 0.4070 10.87 A115900200226 11.09 0.5965 9.54 A115900200227 11.09 0.7586 9.34 A115900200228 11.09 0.8813 11.71 A115900200229 11.09 0.9630 14.80 A115900200230 11.09 0.9957 15.83 A115900200231 11.40 -0.9421 35.45 A115900200232 11.40 -0.8903 27.32 A115900200233 11.40 -0.8262 20.21 A115900200234 11.40 -0.7376 14.04 A115900200235 11.40 -0.6312 9.21 A115900200236 11.40 -0.5045 8.18 A115900200237 11.40 -0.3532 8.60 A115900200238 11.40 -0.1802 10.36 A115900200239 11.40 0.0133 10.88 A115900200240 11.40 0.2123 10.89 A115900200241 11.40 0.4085 9.55 A115900200242 11.40 0.5966 9.05 A115900200243 11.40 0.7601 9.05 A115900200244 11.40 0.8841 11.01 A115900200245 11.40 0.9659 14.72 A115900200246 11.40 0.9945 15.96 A115900200247 11.91 -0.9441 29.00 A115900200248 11.91 -0.8924 24.68 A115900200249 11.91 -0.8270 18.72 A115900200250 11.91 -0.7426 12.96 A115900200251 11.91 -0.6336 9.15 A115900200252 11.91 -0.5055 8.43 A115900200253 11.91 -0.3528 8.93 A115900200254 11.91 -0.1798 9.96 A115900200255 11.91 0.0138 11.49 A115900200256 11.91 0.2127 11.48 A115900200257 11.91 0.4103 10.03 A115900200258 11.91 0.5984 9.41 A115900200259 11.91 0.7605 9.51 A115900200260 11.91 0.8859 11.66 A115900200261 11.91 0.9691 15.66 A115900200262 11.91 0.9950 17.10 A115900200263 12.40 -0.9429 30.09 A115900200264 12.40 -0.8925 24.64 A115900200265 12.40 -0.8258 17.13 A115900200266 12.40 -0.7414 11.37 A115900200267 12.40 -0.6324 7.98 A115900200268 12.40 -0.5043 7.46 A115900200269 12.40 -0.3516 8.17 A115900200270 12.40 -0.1785 9.50 A115900200271 12.40 0.0150 10.21 A115900200272 12.40 0.2112 10.62 A115900200273 12.40 0.4115 9.37 A115900200274 12.40 0.5982 8.85 A115900200275 12.40 0.7631 9.46 A115900200276 12.40 0.8858 12.03 A115900200277 12.40 0.9690 16.24 A115900200278 12.40 0.9921 17.57 A115900200279 12.90 -0.9417 25.42 A115900200280 12.90 -0.8927 20.18 A115900200281 12.90 -0.8260 13.49 A115900200282 12.90 -0.7374 8.97 A115900200283 12.90 -0.6311 7.01 A115900200284 12.90 -0.4990 7.00 A115900200285 12.90 -0.3490 7.92 A115900200286 12.90 -0.1719 9.77 A115900200287 12.90 0.0189 10.17 A115900200288 12.90 0.2179 9.65 A115900200289 12.90 0.4168 9.12 A115900200290 12.90 0.6035 9.12 A115900200291 12.90 0.7671 9.83 A115900200292 12.90 0.8884 12.50 A115900200293 12.90 0.9729 17.43 A115900200294 12.90 0.9961 18.35 A115900200295 ENDDATA 267 0 A115900200296 ENDSUBENT 295 0 A115900299999 SUBENT A1159003 20210125 A096A115900300001 BIB 5 15 A115900300002 REACTION (1-H-3(P,N)2-HE-3,,DA,,LEG/1K2) A115900300003 COMMENT 1K2 - modifier for Legendre or cos coefficients of A115900300004 the form k**2 d-sig/d-omega = sum(a(l)*p(l)), where A115900300005 k = wave-vector A115900300006 SAMPLE The tritium gas was contained in a thin-walled steel A115900300007 cylinder 2 cm long and 0.6 cm in diam. Target A115900300008 pressures were such that the tritium gas caused 5 and A115900300009 13 MeV protons to lose 40 and 30 keV of energy, A115900300010 respectively. A115900300011 STATUS (CURVE) fig 6 from Nucl.Phys.,27(1961)421 A115900300012 (fig.11, 12 in Wilson's thesis) A115900300013 Energy values were taken from the text on the fig.5 A115900300014 (COREL,A1190004) angular distributions A115900300015 HISTORY (20210125A) SD: SF9=EXP deleted from REACTION code. A115900300016 Data re-digitized. BIB updated. A115900300017 ENDBIB 15 0 A115900300018 COMMON 1 3 A115900300019 ERR-DIG A115900300020 NO-DIM A115900300021 0.0028 A115900300022 ENDCOMMON 3 0 A115900300023 DATA 3 84 A115900300024 NUMBER-CM EN DATA-CM A115900300025 NO-DIM MEV NO-DIM A115900300026 0. 4.94 0.4018 A115900300027 0. 5.44 0.3983 A115900300028 0. 5.94 0.3878 A115900300029 0. 6.44 0.3819 A115900300030 0. 6.94 0.3868 A115900300031 0. 7.43 0.3909 A115900300032 0. 7.93 0.4065 A115900300033 0. 8.45 0.3952 A115900300034 0. 8.93 0.3970 A115900300035 0. 9.42 0.3950 A115900300036 0. 9.92 0.4236 A115900300037 0. 10.42 0.3710 A115900300038 0. 11.09 0.3782 A115900300039 0. 11.41 0.3891 A115900300040 0. 11.91 0.3817 A115900300041 0. 12.40 0.3819 A115900300042 0. 12.90 0.3699 A115900300043 1. 4.94 -0.2820 A115900300044 1. 5.44 -0.3048 A115900300045 1. 5.94 -0.2954 A115900300046 1. 6.44 -0.2976 A115900300047 1. 6.94 -0.3112 A115900300048 1. 7.43 -0.3034 A115900300049 1. 7.93 -0.3216 A115900300050 1. 8.45 -0.2802 A115900300051 1. 8.93 -0.2655 A115900300052 1. 9.42 -0.2340 A115900300053 1. 9.92 -0.2468 A115900300054 1. 10.42 -0.1420 A115900300055 1. 11.09 -0.1181 A115900300056 1. 11.41 -0.1516 A115900300057 1. 11.91 -0.1041 A115900300058 1. 12.40 -0.0955 A115900300059 1. 12.90 -0.0358 A115900300060 2. 4.94 0.4886 A115900300061 2. 5.44 0.4933 A115900300062 2. 5.94 0.4833 A115900300063 2. 6.44 0.4695 A115900300064 2. 6.94 0.4649 A115900300065 2. 7.43 0.4503 A115900300066 2. 7.93 0.4380 A115900300067 2. 8.45 0.3957 A115900300068 2. 8.93 0.3726 A115900300069 2. 9.42 0.3264 A115900300070 2. 9.92 0.3218 A115900300071 2. 10.42 0.2333 A115900300072 2. 11.09 0.2149 A115900300073 2. 11.41 0.2565 A115900300074 2. 11.91 0.2234 A115900300075 2. 12.40 0.2565 A115900300076 2. 12.90 0.2181 A115900300077 3. 4.94 -0.1500 A115900300078 3. 5.44 -0.1940 A115900300079 3. 5.94 -0.2395 A115900300080 3. 6.44 -0.2719 A115900300081 3. 6.94 -0.3127 A115900300082 3. 7.43 -0.3335 A115900300083 3. 7.93 -0.3543 A115900300084 3. 8.45 -0.3410 A115900300085 3. 8.93 -0.3479 A115900300086 3. 9.42 -0.3223 A115900300087 3. 9.92 -0.3369 A115900300088 3. 10.42 -0.2594 A115900300089 3. 11.09 -0.2230 A115900300090 3. 11.41 -0.2585 A115900300091 3. 11.91 -0.2127 A115900300092 3. 12.40 -0.2212 A115900300093 3. 12.90 -0.1700 A115900300094 4. 4.94 0.0335 A115900300095 4. 5.44 0.0452 A115900300096 4. 5.94 0.0708 A115900300097 4. 6.44 0.0932 A115900300098 4. 6.94 0.1287 A115900300099 4. 7.43 0.1382 A115900300100 4. 7.93 0.1836 A115900300101 4. 8.45 0.1800 A115900300102 4. 8.93 0.2071 A115900300103 4. 9.42 0.2089 A115900300104 4. 9.92 0.2405 A115900300105 4. 10.42 0.2178 A115900300106 4. 11.09 0.2258 A115900300107 4. 11.41 0.2765 A115900300108 4. 12.40 0.2916 A115900300109 4. 12.90 0.2964 A115900300110 ENDDATA 86 0 A115900300111 ENDSUBENT 110 0 A115900399999 SUBENT A1159004 20210125 A096A115900400001 BIB 7 17 A115900400002 REACTION (1-H-3(P,N)2-HE-3,,SIG) A115900400003 SAMPLE The tritium gas was contained in a thin-walled steel A115900400004 cylinder 2 cm long and 0.6 cm in diam. Target A115900400005 pressures were such that the tritium gas caused 5 and A115900400006 13 MeV protons to lose 40 and 30 keV of energy, A115900400007 respectively. A115900400008 ANALYSIS (INTAD) A115900400009 ERR-ANALYS (DATA-ERR) Error from graphic bars (in a few points) A115900400010 A11 data presented on the fig. have an accuracy of 10%.A115900400011 REL-REF (A,A0152002,J.D.Seagrave,C,59LONDON,,583,1959) Data A115900400012 from Perry and et. al. presented by J.D.Seagrave A115900400013 STATUS (CURVE) Fig. 7 from Nucl.Phys.,27(1961)421 A115900400014 (fig.13 in Wilson's thesis) A115900400015 Energy values were taken from the text on the fig.5 A115900400016 (COREL,A1159003) Legendre coeff. A115900400017 HISTORY (20210123A) SD: SF9=EXP deleted from REACTION code. A115900400018 Data re-digitized. A115900400019 ENDBIB 17 0 A115900400020 COMMON 1 3 A115900400021 ERR-DIG A115900400022 B A115900400023 0.001 A115900400024 ENDCOMMON 3 0 A115900400025 DATA 3 17 A115900400026 EN DATA DATA-ERR A115900400027 MEV B B A115900400028 4.94 0.368 A115900400029 5.44 0.334 A115900400030 5.94 0.298 A115900400031 6.44 0.271 A115900400032 6.94 0.253 A115900400033 7.43 0.239 A115900400034 7.93 0.232 0.021 A115900400035 8.45 0.211 A115900400036 8.93 0.200 A115900400037 9.42 0.189 A115900400038 9.92 0.191 A115900400039 10.42 0.160 A115900400040 11.09 0.152 0.015 A115900400041 11.41 0.150 A115900400042 11.91 0.144 A115900400043 12.40 0.133 A115900400044 12.90 0.126 A115900400045 ENDDATA 19 0 A115900400046 ENDSUBENT 45 0 A115900499999 SUBENT A1159005 20210125 A096A115900500001 BIB 7 17 A115900500002 REACTION (1-H-2(D,N+P)1-H-2,,DA,N) A115900500003 SAMPLE (CH2)n A115900500004 REL-REF (A,A1120002,L.Cranberg+,J,PR,104,1639,1956) A115900500005 (A,,J.D.Anderson,W,ANDERSON,1960) The data of A115900500006 Anderson were presented by Brolley in his publication A115900500007 (see J.E.Brolley+, Fast neutron Physics, edited by A115900500008 J.B. Marion+ (Interscience Publishers,Inc., A115900500009 New York,1960), Vol,1, Chap.I.C.) A115900500010 FLAG (1.) Tabulated values from A115900500011 Bull.Am.Phys.Soc.5,410(D6),1960 A115900500012 STATUS (CURVE) Fig 5 from Wilson's thesis A115900500013 Two tabulated values at 8.9 and 12.9 are from the A115900500014 Bul.Amer.Phys.Soc.,Ser.II,Vol.5,Iss.6, p.410 (1960) A115900500015 COMMENT From SD: The digitized values and the tabulated values A115900500016 match within the specified digitization error. A115900500017 HISTORY (20210123T) SD: From prev.compilation (A1305.002 and A115900500018 A1600.003). Data were re-digitized. A115900500019 ENDBIB 17 0 A115900500020 COMMON 3 3 A115900500021 ANG EN-ERR ERR-DIG A115900500022 ADEG MEV MB/SR A115900500023 0. 0.01 0.2 A115900500024 ENDCOMMON 3 0 A115900500025 DATA 3 4 A115900500026 EN DATA FLAG A115900500027 MEV MB/SR NO-DIM A115900500028 8.9 71. 1. A115900500029 9.84 109.0 A115900500030 10.9 133.2 A115900500031 12.9 185. 1. A115900500032 ENDDATA 6 0 A115900500033 ENDSUBENT 32 0 A115900599999 SUBENT A1159006 20210123 A096A115900600001 BIB 5 15 A115900600002 REACTION (1-H-3(P,N+P)1-H-2,,DA,P) A115900600003 SAMPLE The tritium gas was contained in a thin-walled steel A115900600004 cylinder 2 cm long and 0.6 cm in diam. Target A115900600005 pressures were such that the tritium gas caused 5 and A115900600006 13 MeV protons to lose 40 and 30 keV of energy, A115900600007 respectively. A115900600008 COMMENT By authors. Using the spectrometer properties of the A115900600009 counter telescope, an attempt was made to observe the A115900600010 continuum of neutrons from the reaction T(p,np)D. A115900600011 At abombarding energy of 11.9 MeV no neutrons were A115900600012 observed that could definitely be attributed to A115900600013 the reaction and the upper limit placed on the A115900600014 differential cross section at zero degrees is 10 mb/sr.A115900600015 STATUS (TABLE) Text on p.429 of Nucl.Phys.,27(1961)421 A115900600016 HISTORY (20210123T) SD: From prev.compilation (A1600.004). A115900600017 ENDBIB 15 0 A115900600018 NOCOMMON 0 0 A115900600019 DATA 3 1 A115900600020 EN ANG DATA-MAX A115900600021 MEV ADEG MB/SR A115900600022 11.9 0. 10. A115900600023 ENDDATA 3 0 A115900600024 ENDSUBENT 23 0 A115900699999 SUBENT A1159007 20210125 A096A115900700001 BIB 10 28 A115900700002 REACTION (1-H-3(P,N)2-HE-3,,DA) A115900700003 MONITOR (1-H-3(P,N)2-HE-3,,DA) A115900700004 SAMPLE The tritium gas was contained in a thin-walled steel A115900700005 cylinder 2 cm long and 0.6 cm in diam. Target A115900700006 pressures were such that the tritium gas caused 5 and A115900700007 13 MeV protons to lose 40 and 30 keV of energy, A115900700008 respectively. A115900700009 DETECTOR (TELES,PROPC,CSICR) Recoil proton counter telescope. A115900700010 Argon with 5% CO2 was used as the proportional A115900700011 counter gas. The counter wires were .125 mm mo1ybdenum.A115900700012 MONIT-REF (A0152002,J.E.Perry Jr,W,PERRY,1959) - Because A115900700013 the composition of the target gas was unknown in the A115900700014 present case, the present work is a relative A115900700015 measurement of the differential cross section and is A115900700016 normalized to the data of Perry et al. in the region A115900700017 of 5 to 6 MeV. A115900700018 FLAG (1.) Tabulated values from A115900700019 Bull.Am.Phys.Soc.5,410(D6),1960 A115900700020 ERR-ANALYS (ERR-T) Total error shown in a few points on fig. A115900700021 (ERR-1) The error bars shown are +- 7% which is A115900700022 the estimated error of the data of Perry et al. A115900700023 (ERR-S,,2.) Statistical error A115900700024 COMMENT From SD: The digitized values and the tabulated values A115900700025 match within the specified digitization error. A115900700026 STATUS (CURVE) Fig. 1 from Nucl.Phys.,27(1961)421 A115900700027 (same fig.6 in Wilson's thesis and a few values in A115900700028 Bull.Am.Phys.Soc.5,410(D6),1960.) A115900700029 HISTORY (20210123T) SD + few tabulated values from A1600.002. A115900700030 ENDBIB 28 0 A115900700031 COMMON 4 3 A115900700032 ANG ERR-1 EN-ERR-DIG ERR-DIG A115900700033 ADEG PER-CENT MEV MB/SR A115900700034 0. 7.0 0.04 0.3 A115900700035 ENDCOMMON 3 0 A115900700036 DATA 4 18 A115900700037 EN DATA ERR-T FLAG A115900700038 MEV MB/SR MB/SR NO-DIM A115900700039 4.9 67.0 5.3 1. A115900700040 5.39 55.4 A115900700041 5.88 46.5 A115900700042 6.37 39.2 A115900700043 6.87 34.9 A115900700044 7.37 30.5 2.1 A115900700045 7.88 27.6 A115900700046 8.37 27.0 A115900700047 8.89 25.8 A115900700048 9.39 25.5 A115900700049 10.0 26. 1. A115900700050 10.39 26.6 A115900700051 10.91 27.4 2.3 A115900700052 11.43 29.0 4.6 A115900700053 11.94 30.3 A115900700054 12.43 32.3 A115900700055 12.92 34.1 2.5 A115900700056 13.4 36. 1. A115900700057 ENDDATA 20 0 A115900700058 ENDSUBENT 57 0 A115900799999 SUBENT A1159008 20210125 A096A115900800001 BIB 6 13 A115900800002 REACTION (1-H-2(D,N)2-HE-3,,DA) A115900800003 SAMPLE (CH2)n A115900800004 DETECTOR (TELES,PROPC,CSICR) Recoil proton counter telescope. A115900800005 Argon with 5% CO2 was used as the proportional A115900800006 counter gas. The counter wires were .125 mm mo1ybdenum.A115900800007 ERR-ANALYS (ERR-T) Total error (shown in a few points on fig.) A115900800008 includes: A115900800009 (ERR-1) The error due to charge A115900800010 (ERR-2) The error due to pressure A115900800011 (ERR-3) The error due to efficiency calculations A115900800012 (ERR-S,,1.7) Statistical error A115900800013 STATUS (CURVE) Fig. 3 from Wilson's thesis A115900800014 HISTORY (20210125C) SD A115900800015 ENDBIB 13 0 A115900800016 COMMON 7 6 A115900800017 ANG ERR-1 ERR-2 ERR-3 ERR-T EN-ERR-DIG A115900800018 ERR-DIG A115900800019 ADEG PER-CENT PER-CENT PER-CENT PER-CENT MEV A115900800020 MB/SR A115900800021 0. 1. 1. 2.5 6. 0.004 A115900800022 0.07 A115900800023 ENDCOMMON 6 0 A115900800024 DATA 2 18 A115900800025 EN DATA A115900800026 MEV MB/SR A115900800027 4.784 72.93 A115900800028 5.382 82.83 A115900800029 5.912 83.72 A115900800030 6.383 88.34 A115900800031 6.893 93.07 A115900800032 7.442 93.19 A115900800033 7.874 93.85 A115900800034 8.404 94.96 A115900800035 8.876 95.41 A115900800036 9.425 100.80 A115900800037 9.926 97.73 A115900800038 10.466 101.26 A115900800039 10.957 99.28 A115900800040 11.467 98.96 A115900800041 11.948 102.93 A115900800042 12.459 101.29 A115900800043 12.950 101.40 A115900800044 13.264 101.41 A115900800045 ENDDATA 20 0 A115900800046 ENDSUBENT 45 0 A115900899999 ENDENTRY 8 0 A115999999999