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/* NRDF D1853 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
D#=D1853;
TITLE=/ Mass separation of neutron-rich isotopes using a gas-jet
coupled thermal ion source /;
PURPOSE=/ To report on the design and performance of the gas-jet
coupled thermal ion source installed in the JAERI-ISOL /;
ATH=(S.ICHIKAWA'1', M.ASAI'2', K.TSUKADA'1', A.OSA'3', T.IKUTA'2',
N.SHINOHARA'1', H.IIMURA'1', Y.NAGAME'1', Y.HATSUKAWA'1',
I.NISHINAKA'1', K.KAWADE'4', H.YAMAMOTO'4', M.SHIBATA'4',
Y.KOJIMA'4');
INST-ATH=(2JPNJAE'1', 2JPNNAG'2', 2JPNJAE'3', 2JPNNAG'4');
/* '1' Department of Radioisotopes */
/* '2' Department of Nuclear Engineering */
/* '3' Department of Radioisotopes (Takasaki Establishment) */
/* '4' Department of Energy Engineering and Science */
REF=NIM/A;
VLP=374(1996)330;
RCTS=(238U(P,FISSN), 238U(P,FISSN)140CS, 238U(P,FISSN)144CS,
238U(P,FISSN)144BA, 238U(P,FISSN)144LA, 238U(P,FISSN)148LA,
238U(P,FISSN)148CE, 238U(P,FISSN)148PR, 238U(P,FISSN)152ND,
238U(P,FISSN)156PM, 238U(P,FISSN)160EU);
PHQS=XSECTN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,5;
/* 2003-11-05 : Converted, R.Suzuki + N.Otuka. Data converted from
EXFOR O0747 */
RTY=FISSN;
PHQ=XSECTN;
/* Additional results shown but not compiled
- The first observation of a new isotope 166Tb was carried out
using its monoxide ions. Half-life of 166Tb is 21+-6 sec.
Separation efficiency was reported.
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=1.1MG/CM**2;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDGT;
INST-ACC=2JPNJAE;
INC-ENGY-LAB-RANGE=15MEV;
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
/* Experimental Method:
- On-line mass separation (Gas-jet coupled thermal ion source was
installed in the isotope separator on line.)
- Gamma ray spectrometry
/* By authors: Reaction yield was evaluated by the reaction cross
section and correction made, if necessary for the charge
distribution by assuming a Gaussian charge distribution with the
most probable distribution Z(p) of the unchanged charge
distribution model. */
RCT=238U(P,FISSN)144LA;
DET-PARTCL=GAMMA'12';
/* '12' Delayed gamma from 144La */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
INC-ENGY-LAB=15MEV;
ENGY-GAMMA=397.4KEV'13';
INTNSTY-GAMMA=0.943'13';
HALF-LIFE=40.8SEC'13';
/* '13' Delayed gamma from 144La */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
XSECTN
(MB)
8.3
\END;
/*===================================================================*/
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