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6) 8) PRESEND EXPERIMENT 9) DU TOIT ET AL.,Z.PHYS. 246(1971)170. AS CORRECTED WITH S=5.6+-0.6 EV FOR THE E(P)=640 KEV RESONANCE. 10) ERR-ANALYS: ERROS ARE OF THE ORDER OF 25 %, WHICH IS DUE TO UNCERTAINTIES IN THE AREAS OF THE RESONANCE PEAKS,THE RELATIVE EFFICIENCYOF THE NAI DETECTOR AND THE STRENGTH OF THE E(P)=1280 KEV RESONANCE. 14) CALCULATED FROM INCIDENT ENERGY OF PROTON IN \\DATA,1; AND Q-VALUE=8792.5+-0.9KEV(REF., A.H.WAPSTRA ET AL., ATOMIC DATA AND NUCL. DATA TABLES 19 (1977)175. 15) REF.,P.M.ENDT AND C.VAN DER LEUN, NUCL.PHYS.,TO BE PUBLISHED, UNLESS OTHERWISE INDICATED. 16) PRESENT EXPERIMENT 19) ENERGIES WITH ERRORS ARE FROM PRESENT EXPERIMENT; FOR REMAINDERSEE REF.,P.M.ENDT AND C.LEUN, NUCL.PHYS., TO BE PUBLISHED. 36) PRESENT EXPERIMENTAL DETERMINATION FO SPIN-PARITY. 41) DOPPLER SHIFT ATTENUATION FACTOR,F, DEFINED AS THE RATIO OF THEOBSERVED SHIFT AND THE FULL SHIFT. 43) REF., A.ANTTILA ET AL., Z.PHYS. A274(1975)227. THE IMPLANATION ENERGY FOR THE 22NE WAS 5 KEV. 44) REF. M.BISTER ET AL., ANN.ACAD.SCI.FENNICAE, SER. AVI(1970)N0.349. THE IMPLANATION ENERGY FOR THE 22NE WAS 60 KEV. 45) PRESENT EXPERIMENT. THE IMPLANATION ENERGY FOR THE 22NE IONS WAS 3 KEV. 48) DETERMINED AT INCIDENT PROTON ENERGY. 50) CORRECTED FOR FINATE SIZE OF DETECTOR. 51) ONLY STATISCAL ERROS ARE GIVEN. 52) LIFETIME ADOPTED. 53) TRANSITION TO THE FOLLOWING STATE FROM THE RESONANCE. 54) CORRECTED FOR FINITE SIZE OF DETECTOR. 55) DATA = ANGULAR DISTRIBUTION COEFFICIENT OF LEGENDRE POLYNOMIALP(L=2). 56) DATA = ANGULAR DISTRIBUTION COEFFICIENT OF LEGENDRE POLYNOMIALP(L=4). 57) DATA = THE QUADRUPOLE/DIPOLE MIXING RATIO 58) ALTERNATIVE SOLUTION