ENTRY C2839 20221021 C283900000001 SUBENT C2839001 20221021 20231011 C283900100001 BIB 9 11 C283900100002 TITLE Energy Levels in Sulfur Nuclei C283900100003 AUTHOR (P.W.Davison) C283900100004 REFERENCE (J,PR,75,757,1949) C283900100005 #doi:10.1103/PhysRev.75.757 C283900100006 INSTITUTE (1USAYAL) C283900100007 FACILITY (CYCLO,1USAYAL) C283900100008 DETECTOR (PROPC) Proportional counters were used for proton C283900100009 detection. C283900100010 SAMPLE H2S gas, gaseous H2S is available in 99.9% pure form. C283900100011 METHOD (COINC) Proton gamma-ray coincidences. C283900100012 HISTORY (20221021C) BP C283900100013 ENDBIB 11 0 C283900100014 NOCOMMON 0 0 C283900100015 ENDSUBENT 14 0 C283900199999 SUBENT C2839002 20221021 20231011 C283900200001 BIB 2 2 C283900200002 REACTION (16-S-0(D,X)1-H-1,,DA/DE,,REL) C283900200003 STATUS (CURVE) Fig. 6, page 761 of J,PR,75,757,1949. C283900200004 ENDBIB 2 0 C283900200005 COMMON 2 3 C283900200006 EN ANG C283900200007 MEV ADEG C283900200008 3.22 0.0 C283900200009 ENDCOMMON 3 0 C283900200010 DATA 2 77 C283900200011 E DATA C283900200012 MEV ARB-UNITS C283900200013 5.143 18.343 C283900200014 5.216 22.815 C283900200015 5.289 28.383 C283900200016 5.319 30.391 C283900200017 5.445 33.952 C283900200018 5.445 32.948 C283900200019 5.491 30.668 C283900200020 5.553 24.556 C283900200021 5.615 18.901 C283900200022 5.669 14.614 C283900200023 5.685 13.884 C283900200024 5.730 12.881 C283900200025 5.806 10.693 C283900200026 5.873 10.147 C283900200027 5.947 12.613 C283900200028 6.004 20.643 C283900200029 6.059 35.517 C283900200030 6.066 36.520 C283900200031 6.130 45.281 C283900200032 6.280 44.919 C283900200033 6.374 33.334 C283900200034 6.414 27.495 C283900200035 6.468 22.843 C283900200036 6.515 19.103 C283900200037 6.515 18.465 C283900200038 6.599 13.448 C283900200039 6.668 9.618 C283900200040 6.745 4.783 C283900200041 6.806 2.413 C283900200042 6.866 2.049 C283900200043 6.963 2.325 C283900200044 7.015 3.786 C283900200045 7.067 4.699 C283900200046 7.135 4.883 C283900200047 7.195 4.246 C283900200048 7.292 4.431 C283900200049 7.352 4.432 C283900200050 7.442 4.343 C283900200051 7.517 3.341 C283900200052 7.578 2.338 C283900200053 7.661 1.337 C283900200054 7.758 0.335 C283900200055 7.818 0.336 C283900200056 7.893 0.247 C283900200057 7.968 0.157 C283900200058 8.036 0.615 C283900200059 8.103 0.799 C283900200060 8.185 1.075 C283900200061 8.238 2.079 C283900200062 8.305 2.993 C283900200063 8.327 3.997 C283900200064 8.393 6.189 C283900200065 8.453 8.471 C283900200066 8.504 12.304 C283900200067 8.504 10.844 C283900200068 8.570 14.952 C283900200069 8.629 18.055 C283900200070 8.719 16.689 C283900200071 8.765 14.956 C283900200072 8.826 11.399 C283900200073 8.896 6.291 C283900200074 8.972 3.282 C283900200075 9.025 1.458 C283900200076 9.107 1.369 C283900200077 9.160 2.191 C283900200078 9.219 2.740 C283900200079 9.279 3.471 C283900200080 9.346 4.476 C283900200081 9.391 5.298 C283900200082 9.473 6.578 C283900200083 9.532 7.400 C283900200084 9.675 7.221 C283900200085 9.766 5.216 C283900200086 9.826 3.118 C283900200087 9.849 2.206 C283900200088 9.895 1.204 C283900200089 9.940 0.384 C283900200090 ENDDATA 79 0 C283900200091 ENDSUBENT 90 0 C283900299999 SUBENT C2839003 20221021 20231011 C283900300001 BIB 2 2 C283900300002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900300003 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900300004 ENDBIB 2 0 C283900300005 COMMON 2 3 C283900300006 ANG Q-VAL C283900300007 ADEG MEV C283900300008 64.0 3.25 C283900300009 ENDCOMMON 3 0 C283900300010 DATA 2 4 C283900300011 EN DATA C283900300012 MEV ARB-UNITS C283900300013 2.636 0.844 C283900300014 2.937 0.665 C283900300015 3.154 0.924 C283900300016 3.375 1.074 C283900300017 ENDDATA 6 0 C283900300018 ENDSUBENT 17 0 C283900399999 SUBENT C2839004 20221021 20231011 C283900400001 BIB 3 4 C283900400002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900400003 ERR-ANALYS (DATA-ERR) Various sources of errors including C283900400004 probable. C283900400005 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900400006 ENDBIB 4 0 C283900400007 COMMON 2 3 C283900400008 ANG Q-VAL C283900400009 ADEG MEV C283900400010 90.0 3.25 C283900400011 ENDCOMMON 3 0 C283900400012 DATA 3 3 C283900400013 EN DATA DATA-ERR C283900400014 MEV ARB-UNITS ARB-UNITS C283900400015 2.634 0.913 0.109 C283900400016 2.932 0.734 0.065 C283900400017 3.154 0.983 0.055 C283900400018 ENDDATA 5 0 C283900400019 ENDSUBENT 18 0 C283900499999 SUBENT C2839005 20221021 20231011 C283900500001 BIB 2 2 C283900500002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900500003 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900500004 ENDBIB 2 0 C283900500005 COMMON 2 3 C283900500006 ANG Q-VAL C283900500007 ADEG MEV C283900500008 64.0 3.61 C283900500009 ENDCOMMON 3 0 C283900500010 DATA 2 4 C283900500011 EN DATA C283900500012 MEV ARB-UNITS C283900500013 2.636 0.617 C283900500014 2.930 0.932 C283900500015 3.156 1.068 C283900500016 3.374 1.029 C283900500017 ENDDATA 6 0 C283900500018 ENDSUBENT 17 0 C283900599999 SUBENT C2839006 20221021 20231011 C283900600001 BIB 3 4 C283900600002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900600003 ERR-ANALYS (DATA-ERR) Various sources of errors including C283900600004 probable. C283900600005 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900600006 ENDBIB 4 0 C283900600007 COMMON 2 3 C283900600008 ANG Q-VAL C283900600009 ADEG MEV C283900600010 90.0 4.28 C283900600011 ENDCOMMON 3 0 C283900600012 DATA 3 3 C283900600013 EN DATA DATA-ERR C283900600014 MEV ARB-UNITS ARB-UNITS C283900600015 2.632 0.533 0.069 C283900600016 2.934 0.732 0.078 C283900600017 3.152 0.952 0.108 C283900600018 ENDDATA 5 0 C283900600019 ENDSUBENT 18 0 C283900699999 SUBENT C2839007 20221021 20231011 C283900700001 BIB 3 4 C283900700002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900700003 ERR-ANALYS (DATA-ERR) Various sources of errors including C283900700004 probable. C283900700005 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900700006 ENDBIB 4 0 C283900700007 COMMON 2 3 C283900700008 ANG Q-VAL C283900700009 ADEG MEV C283900700010 90.0 4.60 C283900700011 ENDCOMMON 3 0 C283900700012 DATA 3 3 C283900700013 EN DATA DATA-ERR C283900700014 MEV ARB-UNITS ARB-UNITS C283900700015 2.631 0.946 0.057 C283900700016 2.928 0.789 0.062 C283900700017 3.147 0.439 0.096 C283900700018 ENDDATA 5 0 C283900700019 ENDSUBENT 18 0 C283900799999 SUBENT C2839008 20221021 20231011 C283900800001 BIB 3 4 C283900800002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900800003 ERR-ANALYS (DATA-ERR) Various sources of errors including C283900800004 probable. C283900800005 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900800006 ENDBIB 4 0 C283900800007 COMMON 2 3 C283900800008 ANG Q-VAL C283900800009 ADEG MEV C283900800010 90.0 5.75 C283900800011 ENDCOMMON 3 0 C283900800012 DATA 3 3 C283900800013 EN DATA DATA-ERR C283900800014 MEV ARB-UNITS ARB-UNITS C283900800015 2.630 0.915 0.137 C283900800016 2.931 0.825 0.108 C283900800017 3.152 0.873 0.094 C283900800018 ENDDATA 5 0 C283900800019 ENDSUBENT 18 0 C283900899999 SUBENT C2839009 20221021 20231011 C283900900001 BIB 3 4 C283900900002 REACTION (16-S-32(D,P)16-S-33,PAR,DA,,REL) C283900900003 ERR-ANALYS (DATA-ERR) Various sources of errors including C283900900004 probable. C283900900005 STATUS (CURVE) Fig. 10, page 764 of J,PR,75,757,1949. C283900900006 ENDBIB 4 0 C283900900007 COMMON 2 3 C283900900008 ANG Q-VAL C283900900009 ADEG MEV C283900900010 90.0 6.48 C283900900011 ENDCOMMON 3 0 C283900900012 DATA 3 3 C283900900013 EN DATA DATA-ERR C283900900014 MEV ARB-UNITS ARB-UNITS C283900900015 2.628 0.686 0.096 C283900900016 2.928 0.539 0.058 C283900900017 3.149 0.756 0.096 C283900900018 ENDDATA 5 0 C283900900019 ENDSUBENT 18 0 C283900999999 SUBENT C2839010 20221021 20231011 C283901000001 BIB 3 14 C283901000002 REACTION (16-S-32(D,P)16-S-33,PAR,SIG) C283901000003 ANALYSIS In order to calculate the cross section of the C283901000004 S32(d,p) S33 reaction, an integral numbers vs. range C283901000005 curve was taken by setting the counting level as low C283901000006 as possible. In this manner was determined the total C283901000007 number of particles corresponding to the end group C283901000008 that were emitted within the solid angle subtended by C283901000009 the counter. Knowing the beam intensity, time of C283901000010 observation, and number of sulfur nuclei in the C283901000011 target volume, one may calculate the cross section C283901000012 for the reaction that leaves the nucleus in the C283901000013 ground state. C283901000014 STATUS (DEP,C2839009) C283901000015 (TABLE) page 764 of J,PR,75,757,1949. C283901000016 ENDBIB 14 0 C283901000017 COMMON 1 3 C283901000018 E-LVL C283901000019 MEV C283901000020 0.0 C283901000021 ENDCOMMON 3 0 C283901000022 DATA 3 1 C283901000023 EN-MIN EN-MAX DATA C283901000024 MEV MEV B C283901000025 2.50 3.50 0.019 C283901000026 ENDDATA 3 0 C283901000027 ENDSUBENT 26 0 C283901099999 SUBENT C2839011 20221021 20231011 C283901100001 BIB 4 22 C283901100002 REACTION (16-S-32(D,P)16-S-33,,SIG,,AV) C283901100003 ANALYSIS Using the information on the relative intensities of C283901100004 the various groups, one may calculate the cross C283901100005 sections for the total reaction. It was noted that C283901100006 for the three longest range groups there is C283901100007 substantial agreement between relative yields as C283901100008 determined from the integral curve and from the C283901100009 peaked curve. Hence, it is perfectly satisfactory - C283901100010 in fact, preferable - to obtain this information from C283901100011 the peaked data which applies to 90 degree C283901100012 observation only inasmuch as the angular distribution C283901100013 of proton intensities is not spherically symmetric. C283901100014 ERR-ANALYS (DATA-ERR) The error in this figure is probably at C283901100015 least 50% and cannot be definitely assigned because C283901100016 many of the errors involved cannot be accurately C283901100017 estimated with the present experimental arrangement. C283901100018 STATUS (DEP,C2839004) C283901100019 (DEP,C2839006) C283901100020 (DEP,C2839007) C283901100021 (DEP,C2839008) C283901100022 (DEP,C2839009) C283901100023 (TABLE) page 765 of J,PR,75,757,1949. C283901100024 ENDBIB 22 0 C283901100025 NOCOMMON 0 0 C283901100026 DATA 4 1 C283901100027 EN-MIN EN-MAX DATA DATA-ERR C283901100028 MEV MEV B PER-CENT C283901100029 2.50 3.50 1.2 50.0 C283901100030 ENDDATA 3 0 C283901100031 ENDSUBENT 30 0 C283901199999 ENDENTRY 11 0 C283999999999