ENTRY C2877 20221207 C226C2877000 1 SUBENT C2877001 20221207 C226C2877001 1 BIB 7 9 C2877001 2 TITLE Study of the Nuclear Reactions Sc45(p,n)Ti45, C2877001 3 Cu63(p,n)Zn63, Cu65(p,n)Zn65, and Zn(p,n)Ga C2877001 4 AUTHOR (R.M.Brugger,T.W.Bonner,J.B.Marion) C2877001 5 REFERENCE (J,PR,100,84,1955) C2877001 6 #doi:10.1103/PhysRev.100.84 C2877001 7 INSTITUTE (1USARIC) C2877001 8 FACILITY (VDG,1USARIC) C2877001 9 DETECTOR (BF3) C2877001 10 HISTORY (20221207C) BP C2877001 11 ENDBIB 9 0 C2877001 12 COMMON 2 3 C2877001 13 ANG-MIN ANG-MAX C2877001 14 ADEG ADEG C2877001 15 0.0 10.0 C2877001 16 ENDCOMMON 3 0 C2877001 17 ENDSUBENT 16 0 C287700199999 SUBENT C2877002 20221207 C226C2877002 1 BIB 4 13 C2877002 2 REACTION (21-SC-45(P,N)22-TI-45,,DA,,AV) C2877002 3 SAMPLE The target used was 120-keV thick to protons of 2.9 C2877002 4 MeV and had a tungsten backing. C2877002 5 METHOD Counter method involves the use of two BF3 counters, C2877002 6 one embedded in a paragon cylinder 5 in. in diameter C2877002 7 and 5 in. in length (modified long counter) and the C2877002 8 second surrounded by a ring of paraffin 0.5 in. thick C2877002 9 and 2 in. in length (slow counter). Both counters C2877002 10 were placed at 0 degree with respect to the direction C2877002 11 of the proton beam and subtended approximately the C2877002 12 same solid angle at the target. C2877002 13 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877002 14 Fig. 3, page 86 of J,PR,100,84,1955. C2877002 15 ENDBIB 13 0 C2877002 16 NOCOMMON 0 0 C2877002 17 DATA 2 66 C2877002 18 EN DATA C2877002 19 MEV MB/SR C2877002 20 2.912 0.279 C2877002 21 2.933 0.458 C2877002 22 2.954 0.682 C2877002 23 2.976 1.042 C2877002 24 2.987 1.313 C2877002 25 3.028 1.442 C2877002 26 3.070 1.618 C2877002 27 3.112 1.793 C2877002 28 3.159 1.922 C2877002 29 3.211 1.959 C2877002 30 3.253 2.043 C2877002 31 3.300 2.217 C2877002 32 3.347 2.755 C2877002 33 3.395 3.157 C2877002 34 3.433 4.014 C2877002 35 3.495 3.868 C2877002 36 3.547 4.133 C2877002 37 3.579 4.355 C2877002 38 3.610 4.486 C2877002 39 3.646 4.162 C2877002 40 3.683 4.384 C2877002 41 3.725 4.922 C2877002 42 3.757 5.417 C2877002 43 3.790 6.048 C2877002 44 3.841 5.677 C2877002 45 3.903 5.712 C2877002 46 3.944 5.387 C2877002 47 3.987 6.290 C2877002 48 4.050 6.325 C2877002 49 4.107 6.452 C2877002 50 4.159 6.353 C2877002 51 4.191 6.576 C2877002 52 4.207 7.164 C2877002 53 4.264 7.246 C2877002 54 4.286 7.697 C2877002 55 4.312 7.465 C2877002 56 4.339 8.279 C2877002 57 4.349 7.823 C2877002 58 4.380 7.954 C2877002 59 4.412 8.313 C2877002 60 4.443 8.353 C2877002 61 4.503 9.753 C2877002 62 4.544 9.746 C2877002 63 4.627 9.779 C2877002 64 4.674 9.635 C2877002 65 4.717 10.401 C2877002 66 4.759 10.894 C2877002 67 4.777 9.300 C2877002 68 4.829 9.383 C2877002 69 4.876 9.557 C2877002 70 4.929 10.276 C2877002 71 4.992 10.402 C2877002 72 5.038 10.077 C2877002 73 5.091 10.523 C2877002 74 5.132 10.198 C2877002 75 5.175 10.828 C2877002 76 5.231 10.319 C2877002 77 5.294 10.900 C2877002 78 5.361 10.253 C2877002 79 5.402 10.337 C2877002 80 5.449 10.375 C2877002 81 5.496 10.368 C2877002 82 5.548 10.587 C2877002 83 5.601 10.942 C2877002 84 5.673 10.703 C2877002 85 5.750 10.327 C2877002 86 ENDDATA 68 0 C2877002 87 ENDSUBENT 86 0 C287700299999 SUBENT C2877003 20221207 C226C2877003 1 BIB 5 8 C2877003 2 REACTION (21-SC-45(P,N)22-TI-45,,DA,,AV) C2877003 3 SAMPLE The target used was 120-keV thick to protons of 2.9 C2877003 4 MeV and had a tungsten backing. C2877003 5 METHOD The yield of neutrons measured by the slow counter C2877003 6 from threshold to 0.070 MeV above threshold. C2877003 7 CORRECTION The yield has been corrected for background. C2877003 8 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877003 9 Fig. 4, page 87 of J,PR,100,84,1955. C2877003 10 ENDBIB 8 0 C2877003 11 NOCOMMON 0 0 C2877003 12 DATA 2 57 C2877003 13 EN DATA C2877003 14 MEV MB/SR C2877003 15 2.906 0.039 C2877003 16 2.907 0.038 C2877003 17 2.909 1.319 C2877003 18 2.910 2.021 C2877003 19 2.911 1.233 C2877003 20 2.913 0.984 C2877003 21 2.914 1.286 C2877003 22 2.915 1.533 C2877003 23 2.917 1.489 C2877003 24 2.919 0.631 C2877003 25 2.921 0.588 C2877003 26 2.923 0.848 C2877003 27 2.924 1.412 C2877003 28 2.926 0.361 C2877003 29 2.927 0.415 C2877003 30 2.929 0.813 C2877003 31 2.930 0.812 C2877003 32 2.932 1.003 C2877003 33 2.933 0.946 C2877003 34 2.935 0.544 C2877003 35 2.937 0.611 C2877003 36 2.939 0.609 C2877003 37 2.940 0.870 C2877003 38 2.942 0.867 C2877003 39 2.944 1.072 C2877003 40 2.945 0.864 C2877003 41 2.947 0.697 C2877003 42 2.948 0.874 C2877003 43 2.950 1.010 C2877003 44 2.952 0.856 C2877003 45 2.953 1.103 C2877003 46 2.955 0.922 C2877003 47 2.956 1.058 C2877003 48 2.958 2.407 C2877003 49 2.958 2.862 C2877003 50 2.959 3.813 C2877003 51 2.960 3.922 C2877003 52 2.961 3.480 C2877003 53 2.962 2.913 C2877003 54 2.963 2.250 C2877003 55 2.963 1.822 C2877003 56 2.964 1.076 C2877003 57 2.966 1.254 C2877003 58 2.967 1.459 C2877003 59 2.968 1.582 C2877003 60 2.970 1.359 C2877003 61 2.971 1.248 C2877003 62 2.973 1.259 C2877003 63 2.974 1.368 C2877003 64 2.976 1.808 C2877003 65 2.977 1.930 C2877003 66 2.979 1.542 C2877003 67 2.980 1.485 C2877003 68 2.983 1.414 C2877003 69 2.984 0.957 C2877003 70 2.986 1.024 C2877003 71 2.987 1.133 C2877003 72 ENDDATA 59 0 C2877003 73 ENDSUBENT 72 0 C287700399999 SUBENT C2877004 20221207 C226C2877004 1 BIB 4 17 C2877004 2 REACTION (29-CU-63(P,N)30-ZN-63,,DA,,AV) C2877004 3 SAMPLE (29-CU-63,ENR=0.9911) The separated isotope of Cu63 C2877004 4 (99.11 percent Cu63) in the form of CuO was obtained C2877004 5 from the Oak Ridge National Laboratory. The CuO was C2877004 6 reduced to metallic copper and targets were made by C2877004 7 evaporating the metal onto weighed aluminum blanks or C2877004 8 onto tungsten blanks. C2877004 9 METHOD Counter method involves the use of two BF3 counters, C2877004 10 one embedded in a paragon cylinder 5 in. in diameter C2877004 11 and 5 in. in length (modified long counter) and the C2877004 12 second surrounded by a ring of paraffin 0.5 in. thick C2877004 13 and 2 in. in length (slow counter). Both counters C2877004 14 were placed at 0 degree with respect to the direction C2877004 15 of the proton beam and subtended approximately the C2877004 16 same solid angle at the target. C2877004 17 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877004 18 Fig. 5, page 87 of J,PR,100,84,1955. C2877004 19 ENDBIB 17 0 C2877004 20 NOCOMMON 0 0 C2877004 21 DATA 2 81 C2877004 22 EN DATA C2877004 23 MEV MB/SR C2877004 24 4.223 0.268 C2877004 25 4.234 0.691 C2877004 26 4.244 1.168 C2877004 27 4.271 1.478 C2877004 28 4.304 1.734 C2877004 29 4.328 2.152 C2877004 30 4.335 2.736 C2877004 31 4.345 2.946 C2877004 32 4.365 2.779 C2877004 33 4.388 2.505 C2877004 34 4.401 2.767 C2877004 35 4.418 3.028 C2877004 36 4.422 3.666 C2877004 37 4.426 4.145 C2877004 38 4.440 4.673 C2877004 39 4.458 3.760 C2877004 40 4.464 3.118 C2877004 41 4.503 5.132 C2877004 42 4.532 4.855 C2877004 43 4.551 4.528 C2877004 44 4.594 6.700 C2877004 45 4.615 8.239 C2877004 46 4.643 6.736 C2877004 47 4.672 6.406 C2877004 48 4.695 6.398 C2877004 49 4.719 6.977 C2877004 50 4.748 6.700 C2877004 51 4.766 7.441 C2877004 52 4.796 7.537 C2877004 53 4.823 8.594 C2877004 54 4.842 8.001 C2877004 55 4.859 8.102 C2877004 56 4.873 8.524 C2877004 57 4.877 9.056 C2877004 58 4.881 9.748 C2877004 59 4.888 10.385 C2877004 60 4.901 9.847 C2877004 61 4.909 8.938 C2877004 62 4.929 9.091 C2877004 63 4.946 9.512 C2877004 64 4.973 10.036 C2877004 65 4.998 11.360 C2877004 66 5.015 11.728 C2877004 67 5.057 14.006 C2877004 68 5.082 12.718 C2877004 69 5.099 13.085 C2877004 70 5.129 13.129 C2877004 71 5.152 13.387 C2877004 72 5.173 14.340 C2877004 73 5.198 15.558 C2877004 74 5.217 14.965 C2877004 75 5.246 14.475 C2877004 76 5.269 15.160 C2877004 77 5.284 13.928 C2877004 78 5.305 14.987 C2877004 79 5.328 17.433 C2877004 80 5.361 16.942 C2877004 81 5.380 16.935 C2877004 82 5.406 18.953 C2877004 83 5.435 18.836 C2877004 84 5.459 16.961 C2877004 85 5.480 17.327 C2877004 86 5.505 16.945 C2877004 87 5.528 18.964 C2877004 88 5.556 17.834 C2877004 89 5.575 17.241 C2877004 90 5.601 19.845 C2877004 91 5.623 21.651 C2877004 92 5.644 19.670 C2877004 93 5.666 19.236 C2877004 94 5.693 19.813 C2877004 95 5.712 21.780 C2877004 96 5.736 22.572 C2877004 97 5.764 21.069 C2877004 98 5.788 21.274 C2877004 99 5.809 20.253 C2877004 100 5.829 20.620 C2877004 101 5.853 21.305 C2877004 102 5.890 21.772 C2877004 103 5.896 18.890 C2877004 104 5.950 19.298 C2877004 105 ENDDATA 83 0 C2877004 106 ENDSUBENT 105 0 C287700499999 SUBENT C2877005 20221207 C226C2877005 1 BIB 4 10 C2877005 2 REACTION (29-CU-63(P,N)30-ZN-63,,DA,,AV) C2877005 3 SAMPLE (29-CU-63,ENR=0.9911) The separated isotope of Cu63 C2877005 4 (99.11 percent Cu63) in the form of CuO was obtained C2877005 5 from the Oak Ridge National Laboratory. The CuO was C2877005 6 reduced to metallic copper and targets were made by C2877005 7 evaporating the metal onto weighed aluminum blanks or C2877005 8 onto tungsten blanks. C2877005 9 METHOD The slow counter measurement. C2877005 10 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877005 11 Fig. 6, page 88 of J,PR,100,84,1955. C2877005 12 ENDBIB 10 0 C2877005 13 NOCOMMON 0 0 C2877005 14 DATA 2 33 C2877005 15 EN DATA C2877005 16 MEV MB/SR C2877005 17 4.213 0.013 C2877005 18 4.214 0.042 C2877005 19 4.215 0.121 C2877005 20 4.216 0.455 C2877005 21 4.217 1.092 C2877005 22 4.218 1.554 C2877005 23 4.220 1.727 C2877005 24 4.221 1.532 C2877005 25 4.222 1.433 C2877005 26 4.223 1.847 C2877005 27 4.225 2.403 C2877005 28 4.227 2.288 C2877005 29 4.228 2.493 C2877005 30 4.231 2.520 C2877005 31 4.232 2.516 C2877005 32 4.234 3.105 C2877005 33 4.238 2.824 C2877005 34 4.239 2.118 C2877005 35 4.241 1.825 C2877005 36 4.243 2.013 C2877005 37 4.246 2.040 C2877005 38 4.247 2.036 C2877005 39 4.249 1.952 C2877005 40 4.251 1.693 C2877005 41 4.253 1.960 C2877005 42 4.255 1.988 C2877005 43 4.257 1.904 C2877005 44 4.260 1.385 C2877005 45 4.265 1.790 C2877005 46 4.271 2.371 C2877005 47 4.275 1.562 C2877005 48 4.280 1.486 C2877005 49 4.285 1.492 C2877005 50 ENDDATA 35 0 C2877005 51 ENDSUBENT 50 0 C287700599999 SUBENT C2877006 20221207 C226C2877006 1 BIB 4 15 C2877006 2 REACTION (29-CU-65(P,N)30-ZN-65,,DA,,AV) C2877006 3 SAMPLE (29-CU-65,ENR=0.982) The separated isotope of Cu65 C2877006 4 (98.2 percent Cu65) in the form of CuO was reduced C2877006 5 to metallic copper and evaporated onto weighed C2877006 6 aluminum disks. C2877006 7 METHOD Counter method involves the use of two BF3 counters, C2877006 8 one embedded in a paragon cylinder 5 in. in diameter C2877006 9 and 5 in. in length (modified long counter) and the C2877006 10 second surrounded by a ring of paraffin 0.5 in. thick C2877006 11 and 2 in. in length (slow counter). Both counters C2877006 12 were placed at 0 degree with respect to the direction C2877006 13 of the proton beam and subtended approximately the C2877006 14 same solid angle at the target. C2877006 15 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877006 16 Fig. 7, page 88 of J,PR,100,84,1955. C2877006 17 ENDBIB 15 0 C2877006 18 NOCOMMON 0 0 C2877006 19 DATA 2 91 C2877006 20 EN DATA C2877006 21 MEV MB/SR C2877006 22 2.175 0.034 C2877006 23 2.202 0.091 C2877006 24 2.224 0.109 C2877006 25 2.247 0.046 C2877006 26 2.270 0.164 C2877006 27 2.312 0.180 C2877006 28 2.339 0.277 C2877006 29 2.369 0.313 C2877006 30 2.411 0.389 C2877006 31 2.434 0.407 C2877006 32 2.469 0.423 C2877006 33 2.500 0.600 C2877006 34 2.556 0.574 C2877006 35 2.576 0.732 C2877006 36 2.610 0.648 C2877006 37 2.653 0.884 C2877006 38 2.676 0.941 C2877006 39 2.714 1.157 C2877006 40 2.744 0.994 C2877006 41 2.786 1.170 C2877006 42 2.818 1.466 C2877006 43 2.860 1.422 C2877006 44 2.882 2.279 C2877006 45 2.940 1.733 C2877006 46 2.952 1.792 C2877006 47 2.954 2.312 C2877006 48 2.972 3.010 C2877006 49 2.992 2.388 C2877006 50 2.998 1.827 C2877006 51 3.032 1.824 C2877006 52 3.054 1.721 C2877006 53 3.070 1.780 C2877006 54 3.086 2.118 C2877006 55 3.109 2.176 C2877006 56 3.139 2.072 C2877006 57 3.166 2.190 C2877006 58 3.178 2.448 C2877006 59 3.185 2.248 C2877006 60 3.198 2.626 C2877006 61 3.244 2.601 C2877006 62 3.259 2.780 C2877006 63 3.279 2.838 C2877006 64 3.305 2.915 C2877006 65 3.331 3.612 C2877006 66 3.346 4.631 C2877006 67 3.355 3.890 C2877006 68 3.387 3.426 C2877006 69 3.409 3.304 C2877006 70 3.427 3.862 C2877006 71 3.453 3.799 C2877006 72 3.482 3.516 C2877006 73 3.514 3.893 C2877006 74 3.527 4.351 C2877006 75 3.555 5.908 C2877006 76 3.576 5.366 C2877006 77 3.586 4.985 C2877006 78 3.615 4.642 C2877006 79 3.646 4.799 C2877006 80 3.677 4.996 C2877006 81 3.701 5.193 C2877006 82 3.722 5.751 C2877006 83 3.747 7.368 C2877006 84 3.767 6.586 C2877006 85 3.790 5.524 C2877006 86 3.815 5.341 C2877006 87 3.828 5.800 C2877006 88 3.856 6.097 C2877006 89 3.866 6.636 C2877006 90 3.888 6.473 C2877006 91 3.915 6.551 C2877006 92 3.932 7.189 C2877006 93 3.951 7.087 C2877006 94 3.970 6.165 C2877006 95 3.988 6.843 C2877006 96 4.011 6.960 C2877006 97 4.037 6.778 C2877006 98 4.046 7.197 C2877006 99 4.073 7.274 C2877006 100 4.096 7.451 C2877006 101 4.109 7.830 C2877006 102 4.135 7.587 C2877006 103 4.149 7.266 C2877006 104 4.173 7.523 C2877006 105 4.185 7.822 C2877006 106 4.209 8.140 C2877006 107 4.222 8.478 C2877006 108 4.250 9.055 C2877006 109 4.267 9.353 C2877006 110 4.289 9.251 C2877006 111 4.304 9.110 C2877006 112 4.332 9.607 C2877006 113 ENDDATA 93 0 C2877006 114 ENDSUBENT 113 0 C287700699999 SUBENT C2877007 20221207 C226C2877007 1 BIB 4 12 C2877007 2 REACTION (30-ZN-0(P,N),,DA,,AV/REL) C2877007 3 SAMPLE A 120-keV natural zinc target. C2877007 4 METHOD Counter method involves the use of two BF3 counters, C2877007 5 one embedded in a paragon cylinder 5 in. in diameter C2877007 6 and 5 in. in length (modified long counter) and the C2877007 7 second surrounded by a ring of paraffin 0.5 in. thick C2877007 8 and 2 in. in length (slow counter). Both counters C2877007 9 were placed at 0 degree with respect to the direction C2877007 10 of the proton beam and subtended approximately the C2877007 11 same solid angle at the target. C2877007 12 STATUS (CURVE,,R.M.Brugger+,J,PR,100,84,1955) C2877007 13 Fig. 8, page 89 of J,PR,100,84,1955. C2877007 14 ENDBIB 12 0 C2877007 15 NOCOMMON 0 0 C2877007 16 DATA 2 37 C2877007 17 EN DATA C2877007 18 MEV ARB-UNITS C2877007 19 2.711 0.052 C2877007 20 2.757 0.060 C2877007 21 2.809 0.054 C2877007 22 2.858 0.072 C2877007 23 2.912 0.070 C2877007 24 2.955 0.098 C2877007 25 3.010 0.115 C2877007 26 3.058 0.114 C2877007 27 3.110 0.127 C2877007 28 3.159 0.130 C2877007 29 3.205 0.153 C2877007 30 3.254 0.171 C2877007 31 3.313 0.194 C2877007 32 3.360 0.197 C2877007 33 3.411 0.200 C2877007 34 3.458 0.223 C2877007 35 3.507 0.241 C2877007 36 3.561 0.249 C2877007 37 3.607 0.287 C2877007 38 3.656 0.285 C2877007 39 3.721 0.337 C2877007 40 3.744 0.351 C2877007 41 3.770 0.369 C2877007 42 3.791 0.398 C2877007 43 3.840 0.450 C2877007 44 3.872 0.523 C2877007 45 3.906 0.566 C2877007 46 3.922 0.619 C2877007 47 3.938 0.672 C2877007 48 3.967 0.774 C2877007 49 3.978 0.861 C2877007 50 4.007 0.885 C2877007 51 4.050 1.123 C2877007 52 4.109 1.356 C2877007 53 4.158 1.574 C2877007 54 4.209 1.773 C2877007 55 4.253 1.992 C2877007 56 ENDDATA 39 0 C2877007 57 ENDSUBENT 56 0 C287700799999 ENDENTRY 7 0 C287799999999