ENTRY C2170 20150820 C152C2170 0 1 SUBENT C2170001 20150820 C152C2170 1 1 BIB 9 29 C2170 1 2 TITLE Nuclear Excitation Functions. I. Na23(d,p)Na24, C2170 1 3 Br81(d,p)Br82, and Br(d,2n)Kr(34 hr.) C2170 1 4 AUTHOR (E.T.Clarke,J.W.Irvine Jr) C2170 1 5 REFERENCE (J,PR,66,231,1944) C2170 1 6 #doi:10.1103/PhysRev.66.231 C2170 1 7 INSTITUTE (1USAMIT) C2170 1 8 FACILITY (CYCLO,1USAMIT) MIT cyclotron. C2170 1 9 SAMPLE Stack of NaBr films obtained by evaporation in vacuum C2170 1 10 on aluminum foil. Each foil was covered above and C2170 1 11 below by 1.7 mg/cm2 aluminum foils, so that the C2170 1 12 thickness of the sodium bromide layer was about 5 C2170 1 13 mg/cm2. C2170 1 14 DETECTOR Mica window beta ray counters. Platinum screen C2170 1 15 cathode ray gamma ray counter. C2170 1 16 METHOD (ACTIV,TTM,CHSEP) Deuteron energy determinations were C2170 1 17 made by measurement of range in aluminum. Detection C2170 1 18 by means of beta-ray emission was chosen as the means C2170 1 19 for obtaining the relative excitation curves of the C2170 1 20 bromine and sodium isotopes. The activities of each C2170 1 21 isotope were measured on a calibrated gamma-ray C2170 1 22 counter which yielded three excitation curves and the C2170 1 23 known absolute disintegration rates and scheme of C2170 1 24 24Na and 82Br. When a volatile or gaseous product is C2170 1 25 formed in a solid target it generally is retained in C2170 1 26 the structure of the solid material. In order to C2170 1 27 liberate the krypton after bombardment had been C2170 1 28 completed, it was necessary only to dissolve the C2170 1 29 foils in water. C2170 1 30 HISTORY (20150820C) BP C2170 1 31 ENDBIB 29 0 C2170 1 32 NOCOMMON 0 0 C2170 1 33 ENDSUBENT 32 0 C2170 199999 SUBENT C2170002 20150820 C152C2170 2 1 BIB 3 3 C2170 2 2 REACTION (11-NA-23(D,P)11-NA-24,,SIG) C2170 2 3 DECAY-DATA (11-NA-24,14.8HR,B-) C2170 2 4 STATUS (CURVE) Fig. 4, page 238. C2170 2 5 ENDBIB 3 0 C2170 2 6 NOCOMMON 0 0 C2170 2 7 DATA 2 28 C2170 2 8 EN DATA C2170 2 9 MEV B C2170 2 10 1.244 0.007 C2170 2 11 1.737 0.028 C2170 2 12 2.147 0.092 C2170 2 13 2.479 0.144 C2170 2 14 2.693 0.177 C2170 2 15 2.810 0.204 C2170 2 16 3.160 0.268 C2170 2 17 3.473 0.320 C2170 2 18 3.531 0.329 C2170 2 19 4.236 0.413 C2170 2 20 4.924 0.455 C2170 2 21 5.536 0.467 C2170 2 22 6.229 0.450 C2170 2 23 6.802 0.452 C2170 2 24 7.338 0.424 C2170 2 25 7.796 0.381 C2170 2 26 8.886 0.341 C2170 2 27 9.898 0.292 C2170 2 28 10.293 0.287 C2170 2 29 10.650 0.279 C2170 2 30 11.028 0.247 C2170 2 31 11.344 0.239 C2170 2 32 11.681 0.226 C2170 2 33 11.999 0.214 C2170 2 34 12.315 0.208 C2170 2 35 12.671 0.210 C2170 2 36 12.987 0.205 C2170 2 37 13.363 0.208 C2170 2 38 ENDDATA 30 0 C2170 2 39 ENDSUBENT 38 0 C2170 299999 SUBENT C2170003 20150820 C152C2170 3 1 BIB 3 3 C2170 3 2 REACTION (35-BR-81(D,P)35-BR-82,,SIG) C2170 3 3 DECAY-DATA (35-BR-82-G,34.0HR,B-) C2170 3 4 STATUS (CURVE) Fig. 4, page 238. C2170 3 5 ENDBIB 3 0 C2170 3 6 NOCOMMON 0 0 C2170 3 7 DATA 2 19 C2170 3 8 EN DATA C2170 3 9 MEV B C2170 3 10 3.497 0.007 C2170 3 11 4.247 0.028 C2170 3 12 4.895 0.080 C2170 3 13 5.541 0.152 C2170 3 14 6.227 0.220 C2170 3 15 6.773 0.315 C2170 3 16 7.324 0.351 C2170 3 17 7.797 0.370 C2170 3 18 9.418 0.360 C2170 3 19 10.347 0.354 C2170 3 20 10.704 0.344 C2170 3 21 11.061 0.319 C2170 3 22 11.356 0.337 C2170 3 23 11.713 0.325 C2170 3 24 12.030 0.313 C2170 3 25 12.327 0.303 C2170 3 26 12.683 0.305 C2170 3 27 13.022 0.266 C2170 3 28 13.316 0.299 C2170 3 29 ENDDATA 21 0 C2170 3 30 ENDSUBENT 29 0 C2170 399999 SUBENT C2170004 20150820 C152C2170 4 1 BIB 4 11 C2170 4 2 REACTION (35-BR-79(D,2N)36-KR-79,,SIG,,REL) C2170 4 3 DECAY-DATA (36-KR-79-G,34.0HR,DG) C2170 4 4 COMMENT Original article does not identify 79Kr as a product, C2170 4 5 it simply states Kr. 79Kr was deduced using half life C2170 4 6 and decay mode information. Authors mention also C2170 4 7 Kr-81 as (possible) product, but this could not C2170 4 8 possibly be measured here, as Kr-81g has half-life of C2170 4 9 229000 yr, and Kr-81m has 13 sec. The production of C2170 4 10 Kr-79 from Br-81 is also excluded, as this would be C2170 4 11 the (d,4n) reaction which has a much higher threshold. C2170 4 12 STATUS (CURVE) Fig. 4, page 238. C2170 4 13 ENDBIB 11 0 C2170 4 14 NOCOMMON 0 0 C2170 4 15 DATA 2 19 C2170 4 16 EN DATA C2170 4 17 MEV ARB-UNITS C2170 4 18 5.553 0.001 C2170 4 19 6.204 0.022 C2170 4 20 6.734 0.068 C2170 4 21 7.304 0.104 C2170 4 22 7.855 0.135 C2170 4 23 8.383 0.198 C2170 4 24 8.872 0.271 C2170 4 25 9.384 0.293 C2170 4 26 9.834 0.351 C2170 4 27 10.282 0.431 C2170 4 28 10.678 0.417 C2170 4 29 11.052 0.432 C2170 4 30 11.347 0.457 C2170 4 31 11.722 0.466 C2170 4 32 12.034 0.512 C2170 4 33 12.351 0.504 C2170 4 34 12.702 0.566 C2170 4 35 13.019 0.552 C2170 4 36 13.354 0.573 C2170 4 37 ENDDATA 21 0 C2170 4 38 ENDSUBENT 37 0 C2170 499999 ENDENTRY 4 0 C217099999999