/*===================================================================*/
 /* NRDF D0399 Data No.2                                              */
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 /* 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);
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 RSD=180W;
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 /* 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;
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