Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Mean values of various quantities.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Average multiplicities of identified hadrons produced in fully hadronic (4Q) and semi-leptonic (2Q) W decays at a centre-of-mass energy of 189 GeV.

Corrected momentum distributions of charged particles for 4Q and 2Q events at a centre-of-mass energy 189 GeV.

The difference (4Q-2*2Q) between the fully hadronic and semileptonic momentum distributions at a centre-of-mass energy 189 GeV.

Corrected momentum distributions of charged particles for 4Q and 2Q events at a centre-of-mass energy 183 GeV.

The difference (4Q-2*2Q) between the fully hadronic and semileptonic momentum distributions at a centre-of-mass energy 183 GeV.

Corrected -LN(1/X) distributions for 4Q and 2Q events, and their difference4Q-2*2Q for a centre-of-mass energy of 189 GeV.

Corrected -LN(1/X) distributions for 4Q and 2Q events, and their difference4Q-2*2Q for a centre-of-mass energy of 183 GeV.

Corrected PT distributions for 4Q and 2Q events, and their difference 4Q-2*2Q for a centre-of-mass energy of 189 GeV.

Corrected PT distributions for 4Q and 2Q events, and their difference 4Q-2*2Q for a centre-of-mass energy of 183 GeV.

LN(1/X) distributions for charged particles and identified hadrons producedin hadronic QQBAR events at a centre-of-mass energy of 189 GeV.

LN(1/X) distributions for charged particles and identified hadrons producedin fully hadronic two W decay events at a centre-of-mass energy of 189 GeV.

LN(1/X) distributions for charged particles and identified hadrons producedin semi-leptonic two W decay events at a centre-of-mass energy of 189 GeV.

LN(1/X) distributions for neutral kaons and lambda particles produced in hadronic QQBAR events at a centre-of-mass energies of 183 and 189 GeV.

SPHERICITY distribution.

PLANARITY distribution.

OBLATENESS distribution.

HEAVY JET Mass distribution in the standard scheme definition.

HEAVY JET Mass distribution in the E scheme definition.

LIGHT JET Mass distribution in the standard scheme definition.

JET MASS DIFFERENCE distribution in the standard scheme definition.

TOTAL JET MASS distribution in the standard scheme definition.

TOTAL JET MASS distribution in the E scheme definition.

Wide Jet Broadening (BMAX) distribution.

Narrow Jet Broadening (BMIN) distribution.

Total Jet Broadening (BTOT) distribution.

Jet Broadening Difference (BDIFF) distribution.

C-PARAMETER distribution.

Integrated 2 Jet rates for YCUT=0.04 (Durham, angle ordered Durham and Cambridge alogrithms) and YCUT = 0.8 (JADE alogrithm).

Integrated 3 Jet rates for YCUT=0.04 (Durham, angle ordered Durham and Cambridge alogrithms) and YCUT = 0.8 (JADE alogrithm).

Integrated Jet Cone Energy Fractions (JCEF) for different anglular intervals.

Integrated values of the Energy Energy Correlations (EEC) for different angular intervals.

Integrated values of the Energy Energy Correlations Asymmetry (AEEC) for different angular intervals.

Mean values of Y23.

Mean values of Thrust related observables.

Mean values of the Jet Broadenings.

Mean values of jet masses in the standard definition scheme.

Mean values of jet masses in the E definition scheme.

Mean values of jet masses in the p definition scheme.

Mean values of the C- and D- Parameter variables.

Rapidity distributions (relative to the thrust axis) for c.m. energies from183 to 196 GeV.

Rapidity distributions (relative to the thrust axis) for c.m. energies from200 to 207 GeV.

LN(1/XP) distributions for c.m. energies from 183 to 196 GeV.

LN(1/XP) distributions for c.m. energies from 200 to 207 GeV.

PTIN distributions for c.m. energies from 183 to 196 GeV.

PTIN distributions for c.m. energies from 200 to 207 GeV.

PTOUT distributions for c.m. energies from 183 to 196 GeV.

PTOUT distributions for c.m. energies from 200 to 207 GeV.

1-THRUST distributions for c.m. energies from 183 to 196 GeV.

1-THRUST distributions for c.m. energies from 200 to 207 GeV.

THRUST-MAJOR distributions for c.m. energies from 183 to 196 GeV.

THRUST-MAJOR distributions for c.m. energies from 200 to 207 GeV.

THRUST-MINOR) distributions for c.m. energies from 183 to 196 GeV.

THRUST-MINOR distributions for c.m. energies from 200 to 207 GeV.

Oblateness distributions for c.m. energies from 183 to 196 GeV.

Oblateness distributions for c.m. energies from 200 to 207 GeV.

Wide Jet Broadening (BMAX) distributions for c.m. energies from 183 to 196 GeV.

Wide Jet Broadening (BMAX) distributions for c.m. energies from 200 to 207 GeV.

Total Jet Broadening (BTOT) distributions for c.m. energies from 183 to 196GeV.

Total Jet Broadening (BTOT) distributions for c.m. energies from 200 to 207GeV.

Jet Broadening Difference (BDIFF) distributions for c.m. energies from 183 to 196 GeV.

Jet Broadening Difference (BDIFF) distributions for c.m. energies from 200 to 207 GeV.

C-PARAMETER distributions for c.m. energies from 183 to 196 GeV.

C-PARAMETER distributions for c.m. energies from 200 to 207 GeV.

D-PARAMETER distributions for c.m. energies from 183 to 196 GeV.

D-PARAMETER distributions for c.m. energies from 200 to 207 GeV.

Heavy Jet Mass distributions in the standard scheme definition for c.m. energies from 183 to 196 GeV.

Heavy Jet Mass distributions in the standard scheme definition for c.m. energies from 200 to 207 GeV.

Heavy Jet Mass distributions in the p scheme definition for c.m. energies from 183 to 196 GeV.

Heavy Jet Mass distributions in the p scheme definition for c.m. energies from 200 to 207 GeV.

Heavy Jet Mass distributions in the E scheme definition for c.m. energies from 183 to 196 GeV.

Heavy Jet Mass distributions in the E scheme definition for c.m. energies from 200 to 207 GeV.

Light Jet Mass distributions in the standard definition for c.m. energies from 183 to 196 GeV.

Light Jet Mass distributions in the standard definition for c.m. energies from 200 to 207 GeV.

Jet Mass Difference distributions from c.m.energies from 183 to 196 GeV.

Jet Mass Difference distributions from c.m.energies from 200 to 207 GeV.

Sphericity distributions for c.m.energies from 183 to 196 GeV.

Sphericity distributions for c.m.energies from 200 to 207 GeV.

Planarity distributions for c.m.energies from 183 to 196 GeV.

Planarity distributions for c.m.energies from 200 to 207 GeV.

Aplanarity distributions for c.m.energies from 183 to 196 GeV.

Aplanarity distributions for c.m.energies from 200 to 207 GeV.

Integral of event shape distribution over the specified interval.

Integral of event shape distribution over the specified interval.

Integral of event shape distribution over the specified interval.

Inclusive charged particle distributions, corrected to final state charged particles.

Rapidity, YS, w.r.t. Sphericity axis distribution. Axis definition is from corrected charged plus neutral particles.

Transverse momentum PTIN w.r.t. the Thrust axis. Axis definition is from corrected charged plus neutral particles.

Transverse momentum PTOUT w.r.t. the Thrust axis. Axis definition is from corrected charged plus neutral particles.

1-Thrust distribution. Axis definition is from corrected charged plus neutral particles.

Thrust Major distribution. Axis definition is from corrected charged plus neutral particles.

Thrust Minor distribution. Axis definition is from corrected charged plus neutral particles.

Oblateness distribution. Axis definition is from corrected charged plus neutral particles.

Wide Hemisphere Broadening, DBMAX. Axis definition is from charged corrected plus neutral particles.

Narrow Hemisphere Broadening, DBMIN. Axis definition is from charged corrected plus neutral particles.

Total Hemisphere Broadening, DBSUM. Axis definition is from charged corrected plus neutral particles.

Difference of the Hemisphere Broadening, DBDIFF. Axis definition is from charged corrected plus neutral particles.

2-jet rate for the Durham Algorithm.

3-jet rate for the Durham Algorithm.

4-jet rate for the Durham Algorithm.

5-jet rate for the Durham Algorithm.

2-jet rate for the Jade Algorithm.

3-jet rate for the Jade Algorithm.

4-jet rate for the Jade Algorithm.

5-jet rate for the Jade Algorithm.

Moments of the Oblateness distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Heavy Jet Mass (MH**2/EVIS**2) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Light Jet Mass (ML**2/EVIS**2) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Jet Mass Differences (MDIFF**2/EVIS**2) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Wide Jet Broadening (BMAX) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Small Jet Broadening (BMIN) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the the Total Jet Broadening (BSUM) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the Jet Broadening Difference (BDIFF) distributions at cm energies 133, 161, 172 and 183 GeV.

Moments of the C-parameter (C-PARAM) distributionss at cm energies 133, 161, 172 and 183 GeV.

Distributions of (1-THRUST) at cm energies 133, 161 and 172 GeV.

Distribution of (1-THRUST) at cm energy 183 GeV.

Distributions of Thrust Major (MAJOR) at cm energies 133, 161 and 172 GeV.

Distribution of Thrust Major (MAJOR) at cm energy 183 GeV.

Distributions of Thrust Minor (MINOR) at cm energies 133, 161 and 172 GeV.

Distribution of Thrust Minor (MINOR) at cm energy 183 GeV.

Distributions of Oblateness at cm energies 133, 161 and 172 GeV.

Distribution of Oblateness at cm energy 183 GeV.

Distributions of Sphericity at cm energies 133, 161 and 172 GeV.

Distribution of Sphericity at cm energy 183 GeV.

Distributions of Planarity at cm energies 133, 161 and 172 GeV.

Distribution of Planarity at cm energy 183 GeV.

Distributions of Aplanarity at cm energies 133, 161 and 172 GeV.

Distribution of Aplanarity at cm energy 183 GeV.

Distributions of the Heavy Jet Masses (MH**2/EVIS**2) at cm energies 133, 161 and 172 GeV.

Distribution of the Heavy Jet Masses (MH**2/EVIS**2) at cm energy 183 GeV.

Distributions of the Light Jet Masses (ML**2/EVIS**2) at cm energies 133, 161 and 172 GeV.

Distribution of the Light Jet Masses (ML**2/EVIS**2) at cm energy 183 GeV.

Distributions of the Jet Mass Differences (MDIFF**2/EVIS**2) at cm energies 133, 161 and 172 GeV.

Distribution of the Jet Mass Differences (MDIFF**2/EVIS**2) at cm energy 183 GeV.

Distributions of the Wide Jet Broadening (BMAX) at cm energies 133, 161 and 172 GeV.

Distribution of the Wide Jet Broadening (BMAX) at cm energy 183 GeV.

Distributions of the Small Jet Broadening (BMIN) at cm energies 133, 161 and 172 GeV.

Distribution of the Small Jet Broadening (BMIN) at cm energy 183 GeV.

Distributions of the Total Jet Broadening (BSUM) at cm energies 133, 161 and 172 GeV.

Distribution of the Total Jet Broadening (BSUM) at cm energy 183 GeV.

Distributions of the Jet Broadening Difference (BDIFF) at cm energies 133, 161 and 172 GeV.

Distribution of the Jet Broadening Difference (BDIFF) at cm energy 183 GeV.

Distributions of the C-parameter (C-PARAM) at cm energies 133, 161 and 172 GeV.

Distribution of the C-parameter (C-PARAM) at cm energy 183 GeV.

Distributions of the D-parameter (D-PARAM) at cm energies 133, 161 and 172 GeV.

Distribution of the D-parameter (D-PARAM) at cm energy 183 GeV.

Three different schemes are used for evaluation of ALPHAS: (C=ALPHAS2) second alphas_s order, (C=NLLA) and (C=ALPHAS2+NLLA). See text of the paper for details. The second systematic (DSYS) error is the scale error.

ALPHAS from the higher energies extrapolated to the Z0 mass. The second systematic (DSYS) error is the scale error.

Measured value of the logarithmic energy slope of the inverse coupling constant.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 0-1 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of pseudorapidity for the PT interval 1-10 GeV in fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity PT interval 0-1.5 in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity PT interval 1.5-5 in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 0-1.5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

Charged particle density as a function of PT in the pseudorapidity region 1.5-5 for fixed Q**2 and X intervals in the HCM frame.

No description provided.

Strong coupling constant ALPHA_S(M_Z) determined from fits of different event variables. The systematic errors represents theoretical uncertaintie The last row is a fit to the combined T_c, T_z and Jet Mass variables with possible correlations between them NOT taken into account.

Fragmentation function for Breit frame energy flow selected events for the current hemisphere as a function ln(1/x). Statistical errors only.

Average charged particle multiplicity using energy flow selection.

Average charged particle multiplicity using total current hemisphere of the Breit frame.

Cross sections and ratio of proton dissociative to elastic cross sections.

Q**2 dependence of RHO0 photoproduction cross sections. Statistical errors only.

Angular distribution of RHO0 production.

Elastic PHI electroproduction cross section.

Elastic PHI photoproduction cross section. Errors are the quadratic sum of the statistics and systematics.

Q**2 dependence of the elastic PHI photoproduction cross section.

Angular distribution of the elastic PHI photoproduction.

RHO0 meson spin density matrix element r(04_00).

The multiplicity of charged hadrons for three intervals of mass of the charged hadron system in the forward region.

The multiplicity of charged hadrons for three intervals of mass of the charged hadron system in the backward region.

The multiplicity of positively charged hadrons for three intervals of mass of the charged hadron system in the full phase space region.

The multiplicity of negatively charged hadrons for three intervals of mass of the charged hadron system in the full phase space region.

Charged particle rapidity spectra for three intervals of the mass of the charged haron system.

The central region charged particle density.

The parameter RHO which relects the correlation between the number of particles in the forward and backward hemisphere.

Current hemisphere fragmentation as a function of Q for the XP range 0.05 to 0.10, to show scaling violations.

Current hemisphere fragmentation as a function of Q for the XP range 0.10 to 0.20, to show scaling violations.

Current hemisphere fragmentation as a function of Q for the XP range 0.20 to 0.30, to show scaling violations.

Current hemisphere fragmentation as a function of Q for the XP range 0.30 to 0.40, to show scaling violations.

Current hemisphere fragmentation as a function of Q for the XP range 0.40 to 0.50, to show scaling violations.

Current hemisphere fragmentation as a function of Q for the XP range 0.40 to 0.50, to show scaling violations.

The average charged multiplicity, and the peak and width of the fragmentation function (in LN(1/XP)) as a function of the mean Q, for the total hemisphere of the Breit frame without the energy flow selection discussed in the text of the paper.

The average charged multiplicity, and the peak and width of the fragmentation function (in LN(1/XP)) as a function of the mean Q, with the energy flow selection, obtained from the Total Current Hemisphere sample.

Invariant charged hadron energy spectrum in the current hemisphere for a mean Q of 5.5. Results are given for all the data and for the energy flow selecteddata.

Invariant charged hadron energy spectrum in the current hemisphere for a mean Q of 19.6. Results are given for all the data and for the energy flow selected data.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 12 to 15 GeV**2.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 15 to 20 GeV**2.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 20 to 40 GeV**2.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 40 to 60 GeV**2.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 60 to 80 GeV**2.

Invariant charged hadron energy spectrum in the current hemisphere for the Q**2 range 80 to 100 GeV**2.

The probability per event of observing a charged hadronic multiplicity of (ULT) in the current hemisphere of the Breit frame (at Q = 4.15 GeV, X=0.00126).

The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 4.53 GeV, X=0.00255).

The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 6.20 GeV, X=0.00158).

The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 7.04 GeV, X=0.00410).

The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 14.5 GeV, X=0.00682).

The probability per event of observing a charged hadronic multiplicity of MULT in the current hemisphere of the Breit frame (at Q = 17.3 GeV, X=0.00234).

Feynman X distribution of charged particles in the gamma*-pomeron CM frame,with positive XL corresponding to the direction of the incoming photon.

PT**2 distribution of charged particles in the gamma*-pomeron CM frame, with positive XL corresponding to the direction of the incoming photon.

'Seagull' plot showing mean PT**2 versus XL.

The value of alpha/s at extrapolated to the Z0 mass.. The first systematic (DSYS) errors is due to the experimental procedures, the second is from the theoretical assumptions made in the determination.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 1.5 to 2.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PT distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle PTMAX distribution in the pseudorapidity interval 0.5 to 1.5.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Charged particle pseudorapidity distribution for PT > 1.0 Gev.

Mean K0 multiplicity as function of W.

Mean multiplicity for LAMBDA production.

Q**2 dependence of the elastic J/PSI photoproduction cross section.

Slope of the elastic J/PSI photoproduction T distribution.

Slope of the elastic J/PSI photoproduction T distribution.

Spin density matrices of the angular distribution in J/PSI electroproduction.

Ratio of longitudinal to transverse J/PSI electroproduction cross section determined under the assumption of SCHC.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10) J/PSI electroproduction cross sections.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

Inclusive and inelastic (MX>10GEV) differential cross section for J/PSI electroproduction.

W dependence of the inclusive and inelastic (Z<0.9) J/PSI photoproduction cross section.

Corrected mean values of the Jet Mass (RHO) distribution as a function of Q.

Corrected mean values of the C-Parameter (C-PARAM) distribution as a function of Q.

Corrected mean values of the Y21 distribution (using Factorisable Jade alogrithm) as a function of Q.

Corrected mean values of the Y21 distribution (using Durham kT alogrithm) as a function of Q.

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised Jet Broadening (B) distribution (w.r.t.current hemisphere axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised (1-THRUST) distribution (w.r.t.max long. momentum axis).

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised Jet Mass (RHO) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised C-Parameter(C-PARAM) distribution.

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Factorisable Jade alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Normalised Y21 distribution (using Durham kT alogrithm).

Spin density matrix elements measured for 3 T values for the 1996 data sample.

Ratio of cross sections for elastic RHO electroproduction by longitudinal and transverse photons.

Measurement of the cos(delta) parameter as a function of Q**2, W and T obtained under the NPE and SCHC approximation from fits to the (cos(theta),chi) distribution.

Measurement of the combination of matrix elements 2r1,11 + r1,00 and 2r5,11+ r5,00.

Slope parameter of the exponential t dependence of six values of Q**2.

Exclusive photoproduction cross section for RHO production.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Cross section for exclusive photoproduction of RHO0 as a function of W for different Q**2 values.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.02 to 0.05.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.05 to 0.1.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.1 to 0.2.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.2 to 0.3.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.3 to 0.4.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.4 to 0.5.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.5 to 0.7.

Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.7 to 1.

The slope of the measured T distribution for elastic PHI meson production.

Full set of spin density matrix elements for elastic electroproduction of PHI mesons for W around 75 GeV.

The value of the combination of matrix elements 2*r^5_{11}+r^{5}_{00} for three Q**2 bins.

Ratio of the longitudinal to transverse cross sections for elastic PHI meson electroproduction.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons with a Soeding-inspired analytic function --- statistical correlations only. Only one half of the (symmetric) matrix is stored.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction off protons, differential in the dipion mass and in bins of $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross sections off protons as a function of energy --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic $\rho^0(770)$ photoproduction cross section off protons as a function of energy (various experiments)

Fit of elastic $\rho^0(770)$ photoproduction cross sections off protons as a function of energy (various experiments) --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction cross section off protons, double-differential in the dipion mass and the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single differential in the momentum transfer $\vert t\vert$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\pi^{+}\pi^{-}$ photoproduction double-differenial cross section off protons, as a function of the dipion mass and the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction off protons, single-differential in the momentum transfer $\vert t\vert$, in bins of the photon-proton energy $W$. The cross section is defined as the integral of the relativistic Breit Wigner resonance in the dipion mass over the range $2m_\pi<m_{\pi\pi}<1.53$ GeV. The tabulated cross sections are $\gamma p$ cross sections but can be converted to $ep$ cross sections using the effective photon flux $\Phi_{\gamma/e}$.

Elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction cross section off protons, single differential in the momentum transfer $\vert t\vert$ and in bins of the photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$. Parameters with subscript "el" and "pd" correspond to elastic and proton-dissociative cross sections, respectively.

Regge fit of elastic ($m_Y=m_p$) and proton-dissociative ($1<m_Y<10$ GeV) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ and photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of $b$-slopes in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$.

Fit of Pomeron trajectories in elastic ($m_Y=m_p$) $\rho^0(770)$ photoproduction single-differential cross sections off protons as a function of momentum transfer $t$ in bins of photon-proton energy $W$ --- statistical correlations coefficients $\rho_{ij}$ only. Only one half of the (symmetric) matrix is stored. Bins are identified by their global bin number.