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| /*===================================================================*/
/* NRDF D1725 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1725;
TITLE=/ Reaction mechanism of 6Li scattering at 600 MeV /;
PURPOSE=/ To study the role of the breakup channels and its feedback
to the elastic scattering at intermediate energy /;
ATH=(K.SCHWARZ'1,2', C.SAMANTA'1,3', M.FUJIWARA'1,6', H.REBEL'2',
R.DE.LEO'4', N.MATSUOKA'1', H.UTSUNOMIYA'5', H.AKIMUNE'6',
I.DAITO'1', H.FUJIMURA'1', F.IHARA'1', K.ISHIBASHI'1', Y.MAEDA'1',
T.YAMANAKA'1', H.YOSHIDA'1', A.OKIHANA'7', T.YOSHIMURA'7',
P.K.J.VAN AARLE'1,8', W.A.T.UIJEN'1,8', M.ITO'9', Y.SAKURAGI'9');
INST-ATH=(2JPNRCN'1', 2GERKFK'2', 3INDSAH'3', 2ITYBAU'4', 2JPNKON'5',
2JPNJAE'6', 2JPNKUE'7', 2NEDENT'8', 2JPNJPN'9');
/* '4' Dipartimento di Fisica */
/* '6' Advanced Science Research Center */
/* '9' Department of Physcics, Osaka City University, Osaka */
REF=EPJ/A;
VLP=7(2000)367;
RCTS=(12C(6LI,6LI)X, 58NI(6LI,6LI)X, 90ZR(6LI,6LI)X, 208PB(6LI,6LI)X,
12C(6LI,ALPHA)X, 58NI(6LI,ALPHA)X, 90ZR(6LI,ALPHA)X,
208PB(6LI,ALPHA)X);
PHQS=(ANGL-DSTRN, X'10', DATA'11', DATA'12');
/* '10' Transverse momentum distribution */
/* '11' Double differential cross section against logitudinal
momentum of alpha. */
/* '12' squared of absolute value of momentum distribution */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
/* 2002-09-27 : Converted, Ay + On. Data converted to EXFOR E1725
ENR=X%;
CHM=ELM;
PHYS-FORM=SLD;
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC'13';
/* '13' Ring Cyclotron */
INST-ACC=2JPNRCN;
INC-ENGY-LAB=100MEV/A;
BEAM-INTNSTY=1NA;
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG'14',MWDC,SCT'15',EDE);
/* '14' Grand Gaiden [M.Fujiwara et al., Nucl.Instr.and Meth.in
Phys.Res.A422(1999)484] */
/* '15' To measure energy loss Delta E and the residual energy E
to particle identification */
/* Experimental Method:
- Particle identification by 'E/Delta E' measurement
/* 2006-08-08 : Altered, At. Re-digitized */
RCT=58NI(6LI,ALPHA)X;
RTY=X'27';
/* '27' inclusive breakup */
PHQ=DATA'28';
/* '28' Double differential cross section against logitudinal
momentum of alpha. */
THK-TGT=(4.00MG/CM**2,5.86MG/CM**2);
DET-PARTCL=ALPHA;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
INC-ENGY-LAB=100MEV/A;
THTL=5.5DEG;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
MOM-LNGTD'29' DATA1'30' DELTA-DATA1'30'
(MEV/C) (UNIT2) (UNIT2)
-8.141E+02 6.967E-03 +-NEGLIGIBLE
-7.687E+02 1.066E-02 +-NEGLIGIBLE
-7.295E+02 1.311E-02 +-NEGLIGIBLE
-6.871E+02 1.680E-02 +-NEGLIGIBLE
-6.433E+02 1.721E-02 +-NEGLIGIBLE
-5.978E+02 1.516E-02 +-NEGLIGIBLE
-5.492E+02 1.516E-02 +-NEGLIGIBLE
-5.006E+02 1.803E-02 +-NEGLIGIBLE
-4.505E+02 2.049E-02 +-NEGLIGIBLE
-3.940E+02 2.500E-02 +-2.869E-03
-3.392E+02 3.156E-02 +-3.279E-03
-2.796E+02 4.426E-02 +-4.508E-03
-2.185E+02 6.230E-02 +-6.557E-03
-1.558E+02 9.303E-02 +-9.426E-03
-8.997E+01 1.549E-01 +-1.557E-02
-2.100E+01 2.311E-01 +-2.336E-02
4.796E+01 1.770E-01 +-1.803E-02
1.185E+02 5.615E-02 +-5.738E-03
1.937E+02 1.434E-02 +-NEGLIGIBLE
2.721E+02 2.049E-03 +-NEGLIGIBLE
\END;
/*===================================================================*/
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