|
| /*===================================================================*/
/* NRDF D1493 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1493;
TITLE=/ Complex fragment distributions in 84Kr+27Al at Elab=10.6
MeV/u /;
ATH=(K.Y.NAKAGAWA'1', Y.H.PU'1', S.C.JEONG'1', T.MIZOTA'1',
Y.FUTAMI'1', S.M.LEE'1', T.NAKAGAWA'2', B.HEUSCH'3', K.IEKI'4',
T.MATSUSE'5');
INST-ATH=(2JPNTSU'1', 2JPNIPC'2', 2FR STR'3', 2JPNRIK'4',
2JPNJPN'5');
/* '1' Institute of Physics */
/* '2' Cyclotron Laboratory */
/* '4' Department of Physics */
/* '5' Faculty of Textile Science and Technology, Shinshu
University, Ueda */
REF=PL/B;
VLP=283(1992)185;
RCTS=27AL(84KR,X)X;
PHQS=XSECTN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2005-11-25 : Converted, Kc + On. Converted to EXFOR E1493 */
/* 2008-12-19 : Altered, On. 002-005 corrected */
PHQ=XSECTN;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=0.61MG/CM**2;
BAC=SELF;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNIPC'6';
/* '6' RIKEN Ring Cyclotron Facility */
INC-ENGY-LAB-RANGE=890MEV;
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(CNTR-TLSCP'7',EDE'8');
/* '7' ASCHRA */
/* '8' To obtain missing charge (Delta Z) */
ANL=STATIST-MODEL'9';
/* '9' Extended Hauser-Feshbacn method (EHFM) */
/* 2006-02-23 : Altered, At. Re-digitized */
/* 2008-12-19 : Altered, On. Atomic numbers corrected to integers
RCT=27AL(84KR,X)X;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=890MEV;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z SIGMA DELTA-SIGMA
(NODIM) (MB) (MB)
3 4.492E+01 +-5.054E+00
4 1.427E+01 +-2.144E+00
5 2.245E+01 +-3.545E+00
6 3.348E+01 +-5.546E+00
7 1.224E+01 +-4.953E+00
8 1.990E+01 +-4.894E+00
9 1.264E+01 +-2.902E+00
10 2.242E+01 +-4.600E+00
11 2.775E+01 +-5.250E+00
12 4.138E+01 +-5.274E+00
13 2.737E+01 +-5.178E+00
14 3.320E+01 +-4.987E+00
15 2.839E+01 +-5.468E+00
16 3.274E+01 +-5.679E+00
17 2.610E+01 +-4.937E+00
18 2.330E+01 +-4.779E+00
19 2.626E+01 +-4.555E+00
20 2.882E+01 +-4.999E+00
21 2.806E+01 +-5.308E+00
22 2.824E+01 +-5.343E+00
23 2.677E+01 +-4.853E+00
24 2.899E+01 +-4.802E+00
25 2.191E+01 +-5.027E+00
26 2.420E+01 +-4.388E+00
27 3.015E+01 +-2.949E+00
28 2.877E+01 +-4.766E+00
29 2.673E+01 +-5.057E+00
30 3.136E+01 +-4.711E+00
\END;
/*===================================================================*/
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