/*===================================================================*/ /* NRDF D0399 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; D#=D399; TITLE=/181TA(P,N,N,GAMMA)180W REACTION/; PURPOSE=/IN VIEW OF THE INTERESTING HIGH-SPIN STATES AND THE OTHER STRUCTURAL PROBLEMS AND DISCREPANCIES IN THE LEVEL STRUCTURE OF 180W, WE HAVE UNDERTAKEN A SECOND STUDY OF THE 181TA(P,N,N,GAMMA)180W REACTION. THIS STUDY HAS ALLOWED MODERATELY HIGH-SPIN STATES TO BE OBSERVED WITH THE SIMULTANEOUS OBSERVATION OF MANY STATES OF RELATIVELY LOWER SPIN./; ATH=(L.G.MANN'1',J.B.CARLSON'1',R.G.LANIER'1',G.L.STRUBLE'1', W.M.BUCKLEY'1',D.W.HEIKKINEN'1',I.D.PROCTOR'1',P.K.SHELINE'1'); INST-ATH=(1USALRL'1'); REF=PR/C; VLP=19(1979)1191; RCTS=(181TA(P,N,N,GAMMA)180W); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,2; ENR=X%; CHM=ELM; THK-TGT=5MG/CM**2; BAC=SELF; POL-TGT=NO; ALGN-TGT=NO; INST-ACC=1USALRL; INC-ENGY-LAB-RANGE=(17MEV); DELTA-INC-ENGY-LAB=XKEV; ERS-PRJ=XKEV; BEAM-INTNSTY=XUA; POL-PRJ=NO; DET-PARTCL=(GAMMA,N); DET-SYS=(GE,X'1'); /*@3@*/ SOLID-ANGL=XMSR; ERS-DET=XKEV'1'; /*@4@*/ ANL=(NILS-MODEL,COLL-MODEL); PHQ=(XSECTN,ANGL-DSTRN,ENGY-GAMMA,INTNSTY-GAMMA); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; RSD=180W; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; DATA1'1' DATA2'2' (KEV) (KEV) 102.5,103.6 X'21' 122.7 X'22' 124.6 X'23' 147.2 X'24' 154.2 X'25' 162.4 X'26' 171.0 X'27' 178.5 X'28' 196.5 X'29' 211.4 X'30' 219.5 X'31' 225.2 X'32' 234.0 X'33' 241.9 X'34' 264.7 X'35' 271.8 X'36' 276.9 X'37' 279.3 X'38' 316.6 X'39' 318,320 X'40' 329.5 X'41' 332.2 X'42' 350.9 X'43' 362.1 X'44' 369.0 X'45' 390.6 X'46' 400,402 X'47' 424.5 X'48' 450.0 X'49' 454.9 X'50' 461.4 X'51' 476.6 X'52' 517.4 X'53' 525.7 X'54' 552 X'55' 571.0 X'56' 619.0 X'57' 669 X'58' 744.8 X'59' 780 X'60' 847 X'61' 879.6 X'62' 895.3 X'63' 902.8 X'64' 951.2 X'65' 969.8 X'66' 979.0 X'67' 984.2 X'68' 988.9 X'69' 994.6 X'70' 1013,1014 X'71' 1022.9 X'72' 1041.4 X'73' 1117.2 X'74' 1129.1 X'75' 1166.7 X'76' 1198.1 X'77' 1230 X'78' 1238.0 X'79' 1243.7 X'80' 1257.2 X'81' 1266.2 X'82' 1356.0 X'83' 1365.5 X'84' 1392.2 X'85' 1447.2 X'86' 1581.2 X'87' \END; /*===================================================================*/ |