SC = BEHREND 87D;
IRN = 1627007;
DG;
DGA = PL 183B, 400;
DGA. = DESY-86-133;
RD;
RDA = PL 183B, 400;
RDA. = DESY-86-133;
R = PL 183B, 400;
COD = PHLTA,B183,400;
TY = JOUR;
D = 1987;
RE = E+ E- --> 2HADRON (HADRONS);
REC = E+ E- --> 2HADRON (HADRONS);
BRV = 1.00000;
MODE = INCL;
MULT = 2;
YN = SIG/SIG(Q=EE-MUMU:QED-POLE);
POINT;
BTM = 14.00 ECM;
PLAB = 191781.,191781.,191781.;
ECM = 14.0000,14.0000,14.0000;
Y = 4.10000,0.110000,0.110000;
YSYS = 2.20000,2.20000;
POINT.;
BTM = 22.00 ECM;
PLAB = 473581.,473581.,473581.;
ECM = 22.0000,22.0000,22.0000;
Y = 3.86000,0.120000,0.120000;
YSYS = 2.10000,2.10000;
POINT.;
BTM = 33.80 ECM;
PLAB = 1.11785E+06,1.11785E+06,1.11785E+06;
ECM = 33.8000,33.8000,33.8000;
Y = 3.73000,0.100000,0.100000;
YSYS = 1.90000,1.90000;
POINT.;
BTM = 38.30 ECM;
PLAB = 1.43531E+06,1.43531E+06,1.43531E+06;
ECM = 38.3000,38.3000,38.3000;
Y = 3.88000,0.100000,0.100000;
YSYS = 1.70000,1.70000;
POINT.;
BTM = 41.50 ECM;
PLAB = 1.68518E+06,1.68518E+06,1.68518E+06;
ECM = 41.5000,41.5000,41.5000;
Y = 4.01000,0.170000,0.170000;
YSYS = 1.80000,1.80000;
POINT.;
BTM = 43.50 ECM;
PLAB = 1.85152E+06,1.85152E+06,1.85152E+06;
ECM = 43.5000,43.5000,43.5000;
Y = 3.95000,8.00000E-02,8.00000E-02;
YSYS = 1.40000,1.40000;
POINT.;
BTM = 44.20 ECM;
PLAB = 1.91159E+06,1.91159E+06,1.91159E+06;
ECM = 44.2000,44.2000,44.2000;
Y = 3.99000,0.100000,0.100000;
YSYS = 1.20000,1.20000;
POINT.;
BTM = 46.00 ECM;
PLAB = 2.07045E+06,2.07045E+06,2.07045E+06;
ECM = 46.0000,46.0000,46.0000;
Y = 4.07000,0.210000,0.210000;
YSYS = 1.90000,1.90000;
POINT.;
BTM = 46.60 ECM;
PLAB = 2.12481E+06,2.12481E+06,2.12481E+06;
ECM = 46.6000,46.6000,46.6000;
Y = 4.18000,0.360000,0.360000;
YSYS = 1.70000,1.70000;
SYS;
SYS-ERR = 1.70000;
CSYS = Total normalization uncertainty;
SYS.;
CSYS = Point-to-point systematic uncertainties are given by YSYS's;
DEN = 00:09:05  19:42:43;
DCH = 04:04:18  12:56:55;
CR = DESY-PETRA-CELLO. Final data on the hadronic R ratio based on an integrated  luminosity of 60.3 1/pb;
CR. = Original data were corrected for all background processes, the detector  a cceptance and QED radiative effects up to ALPHA**3 (F.A. Berends, R. Kleiss,  NP  B228, 537 (1983): QED corrections for ISR, initial and final vertex loops,  vac uum polarization. No weak corrections!);
CR. = We additionally unfold the weak loop contribution from the published R val ues using ZFITTER 6.36 (-0.1% at 22 GeV to -0.5% at 46.6 GeV);
SB = ENCODED 16 APR 2004 BY ZOV;
DS = CORRECTED:EW;
AC = DESY-PETRA;
DE = CELLO;
COL = CELLO Collaboration;
DS. = RAD:FULL;
DS. = RPP-2019;
DS. = RPP-2021;
DSC = Radiative correction includes ISR and vacuum polarisation;
DSC. = QUESTION: rescale using up-to-date total cross section data?;
SB. = UPDATED 27 DEC 2019 BY ZOV;
DS. = EE-2024::FS:2hadron (hadrons)::RAD:full::WEIGHT:::COMMENT:;
DS. = EE-2025::FS:2hadron (hadrons)::RAD:full::WEIGHT:::COMMENT:;
DS. = EE-2026::FS:2hadron (hadrons)::RAD:full::WEIGHT:::COMMENT:;
SB. = UPDATED 07 DEC 2024 BY ZOV;
*E