The inclusive charged particle differential cross section.

The K0 + K0BAR inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

The LAMBDA + LAMBDABAR inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

No description provided.

The K*0 + K*BAR0 inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

The PHI meson inclusive differential cross section. The last line in the table is the integral over the full X range of the measurement.. There is an additional 3.4 PCT normalization error (included in the integral).

Measured differential cross section for the production of charged pions perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of charged pions. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of charged kaons perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of charged kaons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of neutral K* mesonsper Z0 decay into light, charm and bottom quarks separately. The errors given a re the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark production of neutral K* mesons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for proton/antiproton production per Z0decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours arenot included.

The ratios of light to heavy quark production of proton/antiprotons. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to thethree flavours are not included.

Measured differential cross section for lambda/antilambda production per Z0decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours arenot included.

The ratios of light to heavy quark lambda/lambdabar production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for the production of neutral kaons perZ0 decay into light, charm and bottom quarks separately. The errors given are t he sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

The ratios of light to heavy quark for neutral kaon production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Measured differential cross section for phi meson production per Z0 decay into light, charm and bottom quarks separately. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from theunfolding procedure. Systematic errors common to the three flavours are not inc luded.

The ratios of light to heavy quark for phi meson production. The errors given are the sum in quadrature of the statistical errors and those systematic errors arising from the unfolding procedure. Systematic errors common to the three flavours are not included.

Corrected total cross sections per hadronic Z decay, and per decay into light, CQ or BQ primary flavour separately. The errors given are the sum in quadrature of experimental and extrapolation uncertainties.

Differences of total cross sections per hadronic Z decay, between CQ (and BQ) and light quarks decays. The errors given are the sum in quadrature of experimental and extrapolation uncertainties.

The differential cross sections for the production of positive and negativepions in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of positive and negative pions in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of neutral K* and K*BAR mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given arethe sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of neutral K* and K*BAR mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of positive and negativeK mesons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of positive and negative kaons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of proton and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising fromthe light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of protons and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. CCT. = Here QUARK (QUARKBAR) means any light quark (antiquark).

The differential cross sections for the production of lambdas and antilambdas in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are thesum in quadrature of statistical errors and those systematic errors arising fro m the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

The normalized difference between the differential cross sections for the production of protons and antiprotons in light (u,d,s) quark jets from hadronic Z0 decays. The errors given are the sum in quadrature of statistical errors and those systematic errors arising from the light quark tagging and unfolding procedure.. Here QUARK (QUARKBAR) means any light quark (antiquark).

No description provided.

Production rates of continuum at resonance energies.

Production rates of continuum at resonance energies.