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| /*===================================================================*/
/* NRDF D1882 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
D#=D1882;
TITLE=/ Spallation of niobium by 12 GeV protons /;
ATH=(T.TOMINAKA'1', S.BAN'1', H.IKEDA'1', K.KATOH'1', K.KONDO'1',
M.TAKASAKI'1', A.YAMAMOTO'1', H.HIRABAYASHI'1', Y.NARAHARA'2');
INST-ATH=(2JPNLEP'1', 2JPNTSU'2');
/* '2' Institute of Physics */
REF=NP/A;
VLP=414(1984)385;
RCTS=93NB(P,X)X;
PHQS=(XSECTN'3', XSECTN'4', XSECTN);
/* '3' Independent cross section */
/* '4' Cumulative cross section */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,1;
/* 2004-02-28 : Compiled, Kc + On */
/* Related references
- C.M.Lederer et al., LEDERER-7, (1978).
Reference from which data were used (Decay data)
- J.B.Cumming et al., NIM, 180(1981)37.
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=XMG/CM**2'5';
/* '5' 50 micro-meter thick for each stack */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN;
INST-ACC=2JPNKEK;
INC-ENGY-LAB=12GEV;
BEAM-INTNSTY=XUA'6';
/* '6' about 1.2e11 protons/pulse */
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=GE(LI)'7';
/* '7' Resolution is 2.0 keV at 1332 keV. Efficiency is 10 %
relative to 7.6 cm x 7.6 cm NaI. */
/* Experimental Method:
- Irradiation with external beam (Exposed for 3 min)
- Gamma ray spectrometry (Measured commencing at 75 min after the
irradiation and continuing intermittently for 200 days)
RCT=93NB(P,X)X;
PHQ=XSECTN'8';
/* '8' Independent cross section */
DET-PARTCL=GAMMA'9';
/* '9' . Gamma energies and half-lives are not given. */
MONTR-RCT=/ 27AL(P,N,3*P)24NA /;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
INC-ENGY-LAB=12GEV;
SYS-ERR=[10%'10';
/* '10' Uncertainty due to the secondary emission chamber
calibration */
DATA1=28GEV'11';
/* '11' Incident energy for adopted monitor cross section which
is independent between 10 and 28 GeV [J.B. Cumming, Ann. Rev.
Nucl. Sci. 13(1963)261]. */
DATA2=7.92MB;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z A ISOMER XSECTN DELTA-XSECTN'12'
(NODIM) (NODIM) (NODIM) (MB) (MB)
5 7 X 9.72 +-2.56
21 44 1 2.36 +-0.21
21 46 X 2.36 +-0.40
21 47 X 1.32 +-0.46
21 48 X 0.31 +-0.12
23 48 X 2.63 +-0.12
25 54 X 5.26 +-0.56
27 56 X 1.56 +-0.33
27 58 X 6.37 +-1.08
31 66 X 4.01 +-0.48
33 72 X 7.76 +-0.60
33 74 X 2.36 +-0.31
34 75 X 4.17 +-0.86
35 76 X 5.98 +-1.57
35 77 X 10.5 +-1.4
37 82 1 4.70 +-0.75
37 83 X 5.2 +-2.8
37 84 X 2.74 +-0.22
39 86 X 5.74 +-0.41
39 86 1 6.55 +-0.49
39 87 X 2.88 +-0.92
39 88 X 10.9 +-2.3
39 90 1 1.05 +-0.05
41 90 X 12.8 +-4.2
41 92 1 15.6 +-1.4
\END;
/*===================================================================*/
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