ENTRY HV70 0 HV70 0 1 SUBENT HV70 1 0 HV70 1 1 BIB 12 42 HV70 1 2 INSTITUTE (SFHLS) HV70 1 3 REFERENCE (J,PS,1,159,1970) HV70 1 4 AUTHORS (P.HOLMBERG,M.VIITASALO) HV70 1 5 TITLE THE EP = 1146 KEV AND 1151 KEV RESONANCES IN THE HV70 1 6 31P(P,GAMMA)32S REACTION HV70 1 7 FACILITY (VDG) 2.5-MV VAN DE GRAAFF ACCELERATOR, HELSINKI HV70 1 8 UNIVERSITY, HELSINKI, FINLAND. HV70 1 9 INC-PART (P) PROTONS. HV70 1 10 TARGETS ZN3P2 TARGETS WERE PREPARED BY EVAPORATION IN VACUO HV70 1 11 ONTO TANTALUM BACKINGS. HV70 1 12 METHOD PROTONS WERE ACCELERATED WITH A VAN DE GRAAFF HV70 1 13 ACCELERATOR AND DEFLECTED WITH A 90-DEGREE ANALYZING HV70 1 14 MAGNET. THE PROTON ENERGY WAS CALIBRATED BY MEANS OF HV70 1 15 THE NUCLEAR MAGNETIC RESONANCE METHOD. THE PROTON HV70 1 16 BEAM STRENGTH WAS KEPT AT ABOUT 3 MICROAMPS. GAMMA HV70 1 17 RAYS DE-EXCITING THE EP = 1146 KEV AND 1151 KEV HV70 1 18 RESONANCES WERE DETECTED WITH A GE(LI) DETECTOR. HV70 1 19 THE DETECTOR ENERGY AND EFFICIENCY CALIBRATION HV70 1 20 WAS PERFORMED USING 56CO AND IAEA STANDARD GAMMA- HV70 1 21 RAY SOURCES. GAMMA-RAY ANGULAR DISTRIBUTIONS WERE HV70 1 22 MEASURED AT THE RESONANCE PROTON ENERGIES WITH HV70 1 23 A NAI SCINTILLATION DETECTOR PLACED AT 0 DEGREE HV70 1 24 AND 90 DEGREES WITH RESPECT TO THE INCIDENT HV70 1 25 PROTON BEAM. THE CENTER OF THE BEAM SPOT WAS HV70 1 26 CHECKED BY MEASUREMENTS ON THE ISOTROPIC 7.89 MEV HV70 1 27 GAMMA RAY FROM THE 30SI(P,GAMMA)31P REACTION AT HV70 1 28 EP = 620 KEV. THE NAI DETECTOR WAS LOCATED AT A HV70 1 29 DISTANCE OF 13 CM FROM THE TARGET. THE MEASURED HV70 1 30 ANGULAR DISTRIBUTION DATA WERE FITTED WITH EVEN- HV70 1 31 ORDER LEGENDRE POLYNOMIAL EXPANSIONS THAT INCLUDED HV70 1 32 TERMS UP TO FOURTH ORDER. HV70 1 33 DETECTORS (GELI) 38-CM**3 GE(LI) DETECTOR WITH AN ENERGY HV70 1 34 RESOLUTION OF 3.5 KEV FWHM FOR THE 1.332-KEV GAMMA HV70 1 35 RAY IN THE 60NI SPECTRA FROM THE DECAY OF 60CO. HV70 1 36 (SCINT) 5-INCH X 4-INCH NAI(TL) SCINTILLATION HV70 1 37 DETECTOR. HV70 1 38 MONITOR (CI) CURRENT INTEGRATOR. HV70 1 39 CORRECTION THE ANGULAR DISTRIBUTION DATA WERE CORRECTED FOR HV70 1 40 GEOMETRIC ASYMMETRIES. GAMMA-RAY YIELD DATA WERE HV70 1 41 CORRECTED FOR DETECTOR EFFICIENCY. HV70 1 42 ERR-ANALYS ERRORS ARE GIVEN BUT NO DETAILS APPEAR IN THE HV70 1 43 ORIGINAL PAPER. HV70 1 44 ENDBIB 42 HV70 1 45 ENDSUBENT 1 HV70 199999 SUBENT HV70 2 0 HV70 2 1 BIB 2 15 HV70 2 2 REACTION 31P(P,GAMMA)32S HV70 2 3 COMMENTS ANGULAR DISTRIBUTION INFORMATION FOR GAMMA-RAYS HV70 2 4 FROM THE DECAY OF RESONANCES IN 32S EXCITED BY THE HV70 2 5 31P(P,GAMMA)32S REACTION ARE GIVEN. DATA TAKEN FROM HV70 2 6 THE TEXT OF THE ORIGINAL PAPER. EP = RESONANCE HV70 2 7 PROTON ENERGY. EX = RESONANCE EXCITATION ENERGY. HV70 2 8 J-PI = SPIN AND PARITY OF THE RESONANCE. A NEGATIVE HV70 2 9 SIGN INDICATES NEGATIVE PARITY. OTHERWISE PARITY IS HV70 2 10 POSITIVE. EI = INTIAL STATE IN 32S FOR GAMMA-RAY HV70 2 11 TRANSITION. EF = FINAL STATE. EG = GAMMA-RAY ENERGY HV70 2 12 FOR THE OBSERVED TRANSITION. A2 = P2 TERM OF THE HV70 2 13 LEGENDRE-POLYNOMIAL EXPANSION USED TO FIT THE DATA. HV70 2 14 A2-ERR = ERROR IN A2. A4 = P4 TERM OF THE HV70 2 15 LEGENDRE-POLYNOMIAL EXPANSION USED TO FIT THE DATA. HV70 2 16 A4-ERR = ERROR IN A4. HV70 2 17 ENDBIB 15 HV70 2 18 DATA 10 2 HV70 2 19 EP EX JPI EI EF EG HV70 2 20 A2 A2-ERR A4 A4-ERR HV70 2 21 KEV KEV NO-DIM KEV KEV KEV HV70 2 22 NO-DIM NO-DIM NO-DIM NO-DIM HV70 2 23 1146. 9974. 2. 9974. 2230. 7744. HV70 2 24 0.175 0.056 -0.097 0.076 HV70 2 25 1151. 9979. 2. 9979. 2230. 7749. HV70 2 26 0.284 0.066 0.137 0.087 HV70 2 27 ENDDATA 10 HV70 2 28 ENDSUBENT 2 HV70 299999 ENDENTRY 2 HV709999999