SC = ALTHOFF 84F;
IRN = 1153170;
DG;
DGA = ZP C22, 307;
DGA. = DESY-83-130;
RD;
RDA = ZP C22, 307;
R = ZP C22, 307;
COD = ZEPYA,C22,307;
TY = JOUR;
D = 1984;
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 = 12.000,12.000,12.000 ECM;
PLAB = 140900.,140900.,140900.;
ECM = 12.0000,12.0000,12.0000;
Y = 3.80000,0.280000,0.280000;
POINT.;
BTM = 14.000,14.000,14.000 ECM;
PLAB = 191781.,191781.,191781.;
ECM = 14.0000,14.0000,14.0000;
Y = 4.14000,0.300000,0.300000;
POINT.;
BTM = 22.000,22.000,22.000 ECM;
PLAB = 473581.,473581.,473581.;
ECM = 22.0000,22.0000,22.0000;
Y = 3.89000,0.170000,0.170000;
POINT.;
BTM = 25.000,25.000,25.000 ECM;
PLAB = 611546.,611546.,611546.;
ECM = 25.0000,25.0000,25.0000;
Y = 3.71000,0.380000,0.380000;
POINT.;
BTM = 27.500,27.400,27.700 ECM;
PLAB = 739971.,734599.,750773.;
ECM = 27.5000,27.4000,27.7000;
Y = 3.90000,0.320000,0.320000;
POINT.;
BTM = 30.100,29.900,30.100 ECM;
PLAB = 886507.,874765.,886507.;
ECM = 30.1000,29.9000,30.1000;
Y = 3.93000,0.180000,0.180000;
POINT.;
BTM = 31.100,30.500,31.500 ECM;
PLAB = 946390.,910225.,970890.;
ECM = 31.1000,30.5000,31.5000;
Y = 3.65000,0.180000,0.180000;
POINT.;
BTM = 33.200,32.500,33.500 ECM;
PLAB = 1.07851E+06,1.03351E+06,1.09809E+06;
ECM = 33.2000,32.5000,33.5000;
Y = 4.08000,0.190000,0.190000;
POINT.;
BTM = 34.000,33.500,34.500 ECM;
PLAB = 1.13112E+06,1.09809E+06,1.16463E+06;
ECM = 34.0000,33.5000,34.5000;
Y = 4.11000,0.110000,0.110000;
POINT.;
BTM = 34.700,34.500,35.500 ECM;
PLAB = 1.17817E+06,1.16463E+06,1.23312E+06;
ECM = 34.7000,34.5000,35.5000;
Y = 4.07000,9.00000E-02,9.00000E-02;
POINT.;
BTM = 36.100,35.500,36.700 ECM;
PLAB = 1.27516E+06,1.23312E+06,1.31790E+06;
ECM = 36.1000,35.5000,36.7000;
Y = 3.92000,0.190000,0.190000;
POINT.;
BTM = 41.400,38.700,43.100 ECM;
PLAB = 1.67706E+06,1.46545E+06,1.81762E+06;
ECM = 41.4000,38.7000,43.1000;
Y = 4.04000,0.290000,0.290000;
SYS;
SYS-ERR = 4.50000;
CSYS = Total systematic uncertainty;
SYS.;
CSYS = Errors in the table are statistical and point-to-point systematic added i n quadrature;
DEN = 00:09:05  19:42:43;
DCH = 04:04:16  22:09:04;
CR = DESY-PETRA-TASSO Collaboration;
CR. = R values below 32.5 GeV are identical to those given in BRANDELIK et al., PL 113B, 499 (1982);
CR. = Results are fully corrected for acceptance and other detector effects and radiative effects (F.A. Berends, R. Kleiss, NP B177, 237 (1981), NP B178, 141 (1 981): only QED (no weak!) corrections were applied to the original data,  i.e. c orrections for ISR, initial and final loops, vacuum polarization and box diagram  contributions.);
CR. = We additionally corrected the original R values for weak loops using ZFITT ER 6.36. The weak correction evolves from -0.1% at 22 GeV to -0.4 PCT at  41.4 G eV. An angular acceptance |cos(theta)| < 0.82 was assumed for the weak correctio n purposes;
SB = ENCODED 15 APR 2004 BY ZOV;
DS = CORRECTED:EW;
AC = DESY-PETRA;
DE = TASSO;
COL = TASSO 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