The cross section for the process e + e − → multihadrons has been measured at the highest PETRA energies. We measure R (the total cross section in units of the point-like e + e - → μ + μ - cross section) to be 2.9 ± 0.7, 4.0 ± 0.5, 4.6 ± 0.4 and 4.2 ± 0.6 at s of 22, 27.7, 30 and 31.6 GeV, respectively. The observed average multiplicity, together with existing low energy data, indicate a rapid increase in multiplicity with increasing energy
Hadron production by e+e- annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
We report on an analysis of the multiplicity distributions of charged particles produced ine+e− anni...
Hadronic jet production bye + e −-annihilation has been studied in the energy range of 14.0–46.7 GeV...
The cross section for the process e + e − → multihadrons has been measured at the highest PETRA ener...
New results on the multihadron production by electron and positron beams colliding with a total ener...
The mean charged multiplicity as well as its distribution has been measured as a function of c.m. en...
Results are presented on multihadron production by e/sup +/e/sup -/ annihilation from the Mark I and...
The total cross section for the process e+e− → hadrons has been measured in the CM energy range betw...
The total cross section for hadron production by e+e- annihilation has been measured at center-of-ma...
We have observed e+e- hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
We have observed e+e− hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
We have observed e+e- hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
It is now nearly three years since the first e+e- collisions were observed at PETRA, which opened a ...
Hadron production by e+e− annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
Hadron production by e+e- annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
Hadron production by e+e- annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
We report on an analysis of the multiplicity distributions of charged particles produced ine+e− anni...
Hadronic jet production bye + e −-annihilation has been studied in the energy range of 14.0–46.7 GeV...
The cross section for the process e + e − → multihadrons has been measured at the highest PETRA ener...
New results on the multihadron production by electron and positron beams colliding with a total ener...
The mean charged multiplicity as well as its distribution has been measured as a function of c.m. en...
Results are presented on multihadron production by e/sup +/e/sup -/ annihilation from the Mark I and...
The total cross section for the process e+e− → hadrons has been measured in the CM energy range betw...
The total cross section for hadron production by e+e- annihilation has been measured at center-of-ma...
We have observed e+e- hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
We have observed e+e− hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
We have observed e+e- hadrons at C.M. energies of 13 GeV and 17 GeV at PETRA using the TASSO detecto...
It is now nearly three years since the first e+e- collisions were observed at PETRA, which opened a ...
Hadron production by e+e− annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
Hadron production by e+e- annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
Hadron production by e+e- annihilation has been studied for c.m. energies W between 13 and 31.6 GeV....
We report on an analysis of the multiplicity distributions of charged particles produced ine+e− anni...
Hadronic jet production bye + e −-annihilation has been studied in the energy range of 14.0–46.7 GeV...