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 /* NRDF D1822 Data No.8                                              */
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 /* Bibliography                                                      */
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 \\BIB,8;
 D#=D1822;
 TITLE=/Structure of the unbound 11N nucleus by the (3He,6He)
        reaction/;
 PURPOSE=/This experiment was performed in order to confirm the
          energies and widths of the ground state and low-lying levels
          of the unbound 11N in the consideration of a possible halo
          structure in 11N./;
 ATH=(V.GUIMARAES'1', S.KUBONO'2', F.C.BARKER'3', M.HOSAKA'4',
      S.C.JEONG'5', I.KATAYAMA'5', T.MIYACHI'2', T.NOMURA'5',
      M.H.TANAKA'5', Y.FUCHI'5', H.KAWASHIMA'5', S.KATO'6',
      C.C.YUN'7', K.ITO'7', H.ORIHARA'7', T.TERAKAWA'7', T.KISHIDA'8',
      Y.PU'8', S.HAMADA'9', M.HIRAI'10', H.MIYATAKE'5');
 INST-ATH=(3BZLUSP'1', 2JPNTOK'2', 3AULCBR'3', 2JPNJPN'4', 2JPNKEK'5',
           2JPNYMG'6', 2JPNTOH'7', 2JPNIPC'8', 2JPNJAE'9', 2JPNTOK'10');
      /* '1' Instituto de Fisica */
      /* '2' Center for Nuclear Study */
      /* '3' Department of Theoretical Physics, Research School of
            Physical Science and Engineering */
      /* '4' Institute for Molecular Science, Okazaki */
      /* '5' Institute of Particle and Nuclear Studies */
      /* '6' Physics Department */
      /* '7' Cyclotron and Radioisotope Center */
      /* '10' Department of Physics */
 REF=(PR/C'11', RBF'12');
 VLP=(67(2003)064601'11', 33(2003)263'12');
 /* '12' V.Guimaraes et al., Proceedings of the XXV Workshop on
         Nuclear Physics in Brazil (Sao Pedro, 2002) */
 RCTS=14N(3HE,6HE)11N;
 PHQS=(ENGY-SPEC'13', RESN-ENGY'14', ANGL-DSTRN, OPT-POTL-PARA);
 /* '13' 6He energy spectra */
 /* '14' Energy above the 10C+p threshold (decay energy) of the 11N
    reasonance */
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 /* Experimental Conditions                                           */
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 \\EXP,8;
 /* 2003-10-03 : Compiled */
 RTY=PKUP;
 ENR=99.95%;
 CHM=ELM;
 PHYS-FORM=GAS;
 THK-TGT=XMG/CM**2'15';
 /* '15' 14N2 gas target filled to a pressure of about 21 cm Hg */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNTOK'16';
 /* '16' Center for Nuclear Study */
 INC-ENGY-LAB=73.40MEV;
 ERS-PRJ=0.05MEV;
 BEAM-INTNSTY=[0.5UA;
 POL-PRJ=0%;
 DET-PARTCL=6HE;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'17',PROP-CNTR'18',SCT'19',TOF'20',EDE'21');
 /* '17' QDD type spectrograph to analyze 6He and other products
 /* '18' Gas proportinal counter to detect reaction products and
         measure energy loss */
 /* '19' To measure energy and time-of-flight */
 /* '20' ToF was obtained from the time interval between
         cyclotron-rf and fast signal from plastic scintillator. */
 /* '21' E and Delta E are obtained from plastic scintillator and
         proportional counter. */
 ERS-DET=[200KEV'22';
 /* '22' FWHM */
 CALB-DET=/ The known states of 21Mg from 24Mg(3He,6He)21Mg is used for
            energy calibration. /;
 /* Experimental Method:
    - Time-of-flight (ToF was obtained from the time interval between
      cyclotron-rf and fast signal from plastic scintillator.)
    - Particle identification by 'E/Delta E' measurement (E and Delta
      E are obtained from plastic scintillator and proportional
      counter.)
 RCT=14N(3HE,6HE)11N;
 PHQ=ENGY-SPEC'44';
 /* '44' 6He energy spectra */
 ANL=RMTRX-THEORY;
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 /* Descriptive Parameters                                            */
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 \\DATA,8;
 INC-ENGY-LAB=73.40MEV;
 RSD=11N;
 THTL=18.0DEG;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY'45' COUNTS DELTA-COUNTS'46'
 (MEV) (NODIM) (NODIM)
  0.000  4. +-2.00
  0.100  1. +-1.00
  0.200  1. +-1.00
  0.300  3. +-1.73
  0.400  2. +-1.41
  0.500  6. +-2.45
  0.600  2. +-1.41
  0.700  1. +-1.00
  0.800  3. +-1.73
  0.900  3. +-1.73
  1.000  6. +-2.45
  1.100  5. +-2.24
  1.200  14. +-3.74
  1.300  15. +-3.87
  1.400  37. +-6.08
  1.500  29. +-5.39
  1.600  31. +-5.57
  1.700  36. +-6.00
  1.800  41. +-6.40
  1.900  52. +-7.21
  2.000  80. +-8.94
  2.100  91. +-9.54
  2.200  109. +-10.44
  2.300  105. +-10.25
  2.400  93. +-9.64
  2.500  99. +-9.95
  2.600  89. +-9.43
  2.700  66. +-8.12
  2.800  50. +-7.07
  2.900  45. +-6.71
  3.000  43. +-6.56
  3.100  35. +-5.92
  3.200  37. +-6.08
  3.300  45. +-6.71
  3.400  43. +-6.56
  3.500  50. +-7.07
 \END;
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