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DESY-HERA. Measurement of the cross sections for production of events containing a leading neutron with at least 20% of the proton beam energy in E+ P collisions at centre-of-mass energy 300 GeV. The data come from the 1995-97 HERA running period with 27.5 GeV positrons colliding with 820 GeV protons. The data cover a wide range of Q**2 ranging from photoproduction (very low Q**2) to deep inelastic scattering (Q**2 & gt; 4 GeV**2). Fraction of events with a leading neutron at XL = 0.24.

Upper limits at 90% CL for the elements of the extended neutrino mixing matrix |Ue4|^2 and |Umu4|^2 depending on the assumed heavy neutral lepton mass. Upper limits on |U_mu4|^2 vs assumed neutrino mass [MeV].

CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet... N-Jet rates from OPAL collaboration at c.m. energy 183 GeV. Jets define using the CONE alogrithm.

CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet... N-Jet rates from the OPAL collaboration at c.m. energy 133 GeV. Jets define using the JADE/E0 alogrithm.

We present photometric properties and distance measurements of 252 high redshift Type Ia supernovae (0.15

DESY-HERA. Measurement of the cross sections for production of events containing a leading neutron with at least 20% of the proton beam energy in E+ P collisions at centre-of-mass energy 300 GeV. The data come from the 1995-97 HERA running period with 27.5 GeV positrons colliding with 820 GeV protons. The data cover a wide range of Q**2 ranging from photoproduction (very low Q**2) to deep inelastic scattering (Q**2 & gt; 4 GeV**2). The normalized cross section (1/SIG)DSIG/dXL for leading neutrons with THETA < 0.8 mrad with statistical errors only.. For the lowest Q**2 data, the normalization uncertainty is +-5 PCT, and with XL > 0.52 there is a further normalization uncertainty of +-4 PCT.. For the intermediate Q**2 and DIS data the normalization uncertainty is +-4 PCT.

Additional file 9: Fig. S9. Cell sorting analysis of cell viability and transfection efficiency in MCF-7 cells. MCF-7 cells were transfected with the dCas9-TET1_MO plasmid alone (TET_MO) and with gRNA 7 (TETg7_MO). Two days post-transfection, MCF-7 cells were stained with propidium iodide (PI) and cell viability and transfection efficiency were quantified using a FACS flow cytometer (BD Biosciences) with a 488-nm blue laser. In the upper panel, the square shows the PI-negative cells (viable), while in the bottom panel are represented the selection of PI-negative/GFP-positive cells.

CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet... Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the OPAL collaboration at c.m. energy 133 GeV. Jets defined using the DURHAM alogrithm.

CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet... Results for ALPHAS at the Z0 mass from fits of the O(alphas**2) predicitonsfor the 3-jet fractions (R3) for the JADE, DURHAM and CAMBRIDGE schemes. The errors shown are total errors and contain all the statistics and systematics.

CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. This is PART 1 of the record and gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. This is PART 2 and gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. This is PART 3 and gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. This is PART 4 and gives the measured observables using the CAMBRIDGE jet finding alogrithm. PART 5 gives the measured observables using the CONE jet finding alogrithm. Numerical values supplied by P Pfeifenschneider. CERN and DESY. Measurments of jet-multiplicity related observables in E+E- annihilations in the c.m. energy range from 35 to 189 GeV using data taken by the JADE and OPAL experiments. The observables are obtained using the JADE, Durham, Cambridge and cone finding jet alogrithms. The observables measured are the N-jet rates, the mean jet multiplicities, the differential cross sections w.r.t. Yn,n+1 and the differential N-jet fractions. The strong coupling constant ALPHAS is determined at each energy by fits to O(alpha_s**2) calculations, as well as matched O(alpha_s**2) and NLLA predictions to the data.. PART 1 of the record gives the ALPHAS results. PART 2 gives the measured observables using the JADE jet finding alogrithm. PART 3 gives the measured observables using the DURHAM jet finding alogrithm. PART 4 gives the measured observables using the CAMBRIDGE jet... Differential distributions in Ynm (the minimum YCUT for the separation inton and m(=n+1) jets). ) from the JADE collaboration at c.m. energy 44 GeV. Jets defined using the DURHAM alogrithm.