/*===================================================================*/ /* NRDF D1841 Data No.119 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,119; D#=D1841; TITLE=/Shell and odd-even effects on alpha-particle energy spectra from the (p,alpha) reaction on nuclei around neutron number 50/; PURPOSE=/To clarify the shell and odd-even effects on the (p,alpha) reaction/; ATH=(I.KUMABE'1', Y.MITO'1', M.HYAKUTAKE'1', N.KOORI'1', H.SAKAI'1', Y.WATANABE'1'); INST-ATH=(2JPNKYU'1'); /* '1' Department of Nuclear Engineering */ REF=PR/C; VLP=35(1987)467; RCTS=(92MO(P,ALPHA)X, 94MO(P,ALPHA)X, 93NB(P,ALPHA)X, 106PD(P,ALPHA)X, AG(P,ALPHA)X, 90ZR(P,ALPHA)X, 96MO(P,ALPHA)X, 98MO(P,ALPHA)X, 100MO(P,ALPHA)X); PHQS=(ENGY-SPEC, ENGY-SPEC'2'); /* '2' Angular integrated energy spectrum */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,119; /* 2003-11-11 : Converted, Data converted from EXFOR E1303. Numerical data are exchanged with author's one. Many data tables are added. */ CHM=ELM; PHYS-FORM=SLD; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=VDGT; INST-ACC=2JPNKYU; BEAM-INTNSTY=20[300NA'3'; /* '3' Smaller beam currents were used at forward angles in order to reduce the dead time for the detector system. */ POL-PRJ=0%; DET-PARTCL=ALPHA; COINC=NO; ANT-COINC=NO; DET-SYS=SBD'4'; /* '4' To analyze and detect alpha-particle. Used as Delta E-E counter. Silicon surface barrier detectors having thickness of 15 and 300 micro-meter. The energy scale for alpha-particles was calibrated using the position of the alpha-particle peaks leading to the ground states of the residual nucleus for high energy calibration points. Low energy calibration points were obtained using the positions of the alpha-particle peaks leading to low lying states of 13N in the 16O(p,alpha)13N reaction on the oxygen impurities on the targets. */ /* Experimental Method: - Particle identification by 'E/Delta E' measurement (To identify alpha-particles from other reaction products) RCT=92MO(P,ALPHA)X; PHQ=ENGY-SPEC'141'; /* '141' Angular integrated energy spectrum */ ENR=98.27%; THK-TGT=0.506MG/CM**2; INC-ENGY-LAB=18MEV; ANL=(STATIST-MODEL'142',PREEQUI-MODEL'143'); /* '142' Statistical evaporation model [J.M. Blatt and V.F. Weisskopf, Theoretical Physics (Wiley, New York 1952). */ /* '143' See [L. Milazzo-Colli and G.M. Braga-Marcazzan, Nucl. Phys. A210(1973)297] for detail. */ /* Analysis: - Integration of angular distribution /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,119; INC-ENGY-LAB=18MEV; EMT=ALPHA; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; ENGY-EMT-CM-MIN ENGY-EMT-CM-MAX DSIGMA/DE DELTA-DSIGMA/DE'144' (MEV) (MEV) (MB/MEV) (MB/MEV) 9.0000 9.2000 1.7234 +-0.0536 9.2000 9.4000 1.9138 +-0.0467 9.4000 9.6000 2.1494 +-0.0484 9.6000 9.8000 2.6633 +-0.0441 9.8000 10.0000 3.0758 +-0.0544 10.0000 10.2000 3.4567 +-0.0593 10.2000 10.4000 3.7508 +-0.0534 10.4000 10.6000 4.0301 +-0.0543 10.6000 10.8000 4.2909 +-0.0587 10.8000 11.0000 4.5008 +-0.0648 11.0000 11.2000 4.6177 +-0.0583 11.2000 11.4000 4.5210 +-0.0584 11.4000 11.6000 4.5367 +-0.0580 11.6000 11.8000 4.3059 +-0.0564 11.8000 12.0000 4.1519 +-0.0552 12.0000 12.2000 3.6404 +-0.0515 12.2000 12.4000 3.3099 +-0.0490 12.4000 12.6000 2.9484 +-0.0470 12.6000 12.8000 2.7719 +-0.0451 12.8000 13.0000 2.5269 +-0.0428 13.0000 13.2000 2.1655 +-0.0397 13.2000 13.4000 1.9404 +-0.0376 13.4000 13.6000 1.6110 +-0.0341 13.6000 13.8000 1.3557 +-0.0311 13.8000 14.0000 0.7648 +-0.0231 14.0000 14.2000 0.8829 +-0.0252 14.2000 14.4000 0.6086 +-0.0208 14.4000 14.6000 0.5723 +-0.0202 14.6000 14.8000 0.8285 +-0.0244 14.8000 15.0000 0.9240 +-0.0252 15.0000 15.2000 0.8432 +-0.0244 15.2000 15.4000 0.1360 +-0.0097 15.4000 15.6000 0.2014 +-0.0121 15.6000 15.8000 0.6859 +-0.0222 15.8000 16.0000 0.2995 +-0.0149 16.0000 16.2000 0.0388 +-0.0052 16.2000 16.4000 0.0278 +-0.0044 16.4000 16.6000 0.0209 +-0.0037 16.6000 16.8000 0.0222 +-0.0039 16.8000 17.0000 0.0184 +-0.0036 17.0000 17.2000 0.0172 +-0.0033 17.2000 17.4000 0.0121 +-0.0028 17.4000 17.6000 0.0119 +-0.0027 17.6000 17.8000 0.0104 +-0.0026 17.8000 18.0000 0.0062 +-0.0020 18.0000 18.2000 0.0105 +-0.0026 18.2000 18.4000 0.0143 +-0.0031 18.4000 18.6000 0.0109 +-0.0028 18.6000 18.8000 0.0097 +-0.0026 18.8000 19.0000 0.0138 +-0.0033 19.0000 19.2000 0.0097 +-0.0026 19.2000 19.4000 0.0099 +-0.0027 19.4000 19.6000 0.0097 +-0.0026 19.6000 19.8000 0.0086 +-0.0025 19.8000 20.0000 0.0096 +-0.0025 20.0000 20.2000 0.0098 +-0.0027 20.2000 20.4000 0.0063 +-0.0022 20.4000 20.6000 0.0023 +-0.0013 20.6000 20.8000 0.0014 +-0.0010 20.8000 21.0000 0.0010 +-0.0007 21.0000 21.2000 0.0010 +-0.0008 21.2000 21.4000 0.0000 +-0.0000 21.4000 21.6000 0.0000 +-0.0000 \END; /*===================================================================*/ |