Mean $p_T$, leading in-jet charged particle.

Mean $p_T$, charged particle jets, $p^{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 5$ GeV, $|\eta^{ch.jet}| < 1.9$.

Charged jet rate, $p^\text{ch.jet}_T > 30$ GeV, $|\eta^{ch.jet}| < 1.9$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $10 < N_\text{ch} \le 30$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $30 < N_\text{ch} \le 50$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $50 < N_\text{ch} \le 80$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $80 < N_\text{ch} \le 110$.

Jet $p_T$ spectrum, $|\eta^{ch.jet}| < 1.9$, $110 < N_\text{ch} \le 140$.

Intrajet ring $p_{T}$ density, $10 < N_\text{ch} \le 30$.

Intrajet ring $p_{T}$ density, $30 < N_\text{ch} \le 50$.

Intrajet ring $p_{T}$ density, $50 < N_\text{ch} \le 80$.

Intrajet ring $p_{T}$ density, $80 < N_\text{ch} \le 110$.

Intrajet ring $p_{T}$ density, $110 < N_\text{ch} \le 140$.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 400 GeV $< p_{\mathrm{T}} <$ 500 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 500 GeV $< p_{\mathrm{T}} <$ 600 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 600 GeV $< p_{\mathrm{T}} <$ 1000 GeV and 0 <|y|< 0.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 20 GeV $< p_{\mathrm{T}} <$ 25 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 25 GeV $< p_{\mathrm{T}} <$ 30 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 30 GeV $< p_{\mathrm{T}} <$ 40 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 400 GeV $< p_{\mathrm{T}} <$ 500 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 500 GeV $< p_{\mathrm{T}} <$ 600 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 600 GeV $< p_{\mathrm{T}} <$ 1000 GeV and 0.5 <|y|< 1.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 20 GeV $< p_{\mathrm{T}} <$ 25 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 25 GeV $< p_{\mathrm{T}} <$ 30 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 30 GeV $< p_{\mathrm{T}} <$ 40 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 400 GeV $< p_{\mathrm{T}} <$ 500 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 500 GeV $< p_{\mathrm{T}} <$ 600 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 600 GeV $< p_{\mathrm{T}} <$ 1000 GeV and 1.0 <|y|< 1.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 20 GeV $< p_{\mathrm{T}} <$ 25 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 25 GeV $< p_{\mathrm{T}} <$ 30 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 30 GeV $< p_{\mathrm{T}} <$ 40 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 400 GeV $< p_{\mathrm{T}} <$ 500 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 500 GeV $< p_{\mathrm{T}} <$ 600 GeV and 1.5 <|y|< 2.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 20 GeV $< p_{\mathrm{T}} <$ 25 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 25 GeV $< p_{\mathrm{T}} <$ 30 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 30 GeV $< p_{\mathrm{T}} <$ 40 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 2.0 <|y|< 2.5. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 20 GeV $< p_{\mathrm{T}} <$ 25 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 25 GeV $< p_{\mathrm{T}} <$ 30 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 30 GeV $< p_{\mathrm{T}} <$ 40 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 40 GeV $< p_{\mathrm{T}} <$ 50 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 50 GeV $< p_{\mathrm{T}} <$ 60 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 60 GeV $< p_{\mathrm{T}} <$ 70 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 70 GeV $< p_{\mathrm{T}} <$ 80 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 80 GeV $< p_{\mathrm{T}} <$ 90 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 90 GeV $< p_{\mathrm{T}} <$ 100 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 100 GeV $< p_{\mathrm{T}} <$ 110 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 110 GeV $< p_{\mathrm{T}} <$ 125 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 125 GeV $< p_{\mathrm{T}} <$ 140 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 140 GeV $< p_{\mathrm{T}} <$ 160 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 160 GeV $< p_{\mathrm{T}} <$ 180 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 180 GeV $< p_{\mathrm{T}} <$ 200 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 200 GeV $< p_{\mathrm{T}} <$ 225 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 225 GeV $< p_{\mathrm{T}} <$ 250 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 250 GeV $< p_{\mathrm{T}} <$ 300 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The measured differential jet shape $\rho(r)$ for jets with 300 GeV $< p_{\mathrm{T}} <$ 400 GeV and 2.5 <|y|< 3.0. The CF in the table refers to unfolding correction factor from {\sc pythia6} Tune Z2. The systematic uncertainties from different sources, jet energy scale (JES), unfolding, and single particle response (SPR), are also presented.

The dependence of $\langle N_\mathrm{ch} \rangle$ on the transverse momentum of jets in two different rapidity regions, $|y| < 1$ and $1 < |y| < 2$.

The dependence of $\langle \delta R^2 \rangle$ on the transverse momentum of jets in two different rapidity regions, $|y| < 1$ and $ 1 < |y| < 2 $.

The dependence of $\langle\delta \eta^2\rangle/\langle\delta \phi^2\rangle$ on the transverse momentum for jets with $|y| < 1$.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 500 to 600 GeV and absolute values of the jet rapidity from 0 to 2.8.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Differential Jet Shape RHO as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 0 to 2.8.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 0 to 0.3.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 0.3 to 0.8.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 0.8 to 1.2.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 1.2 to 2.1.

Measured Integrated Jet Shape 1-PSI as a function of jet transverse momentum for an r value of 0.3 and absolute values of the jet rapidity from 2.1 to 2.8.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 30 to 40 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 40 to 60 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 60 to 80 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 80 to 110 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 110 to 160 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 160 to 210 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 210 to 260 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 2.1 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 260 to 310 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 310 to 400 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0 to 0.3. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0.3 to 0.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0.8 to 1.2. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 1.2 to 2.1. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 400 to 500 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Measured Integrated Jet Shape PSI as a function of r for jet transverse momentum from 500 to 600 GeV and absolute values of the jet rapidity from 0 to 2.8. This is additional data, not in the paper.

Differential cross section for the W range 1.75 to 1.76 GeV.

Differential cross section for the W range 1.76 to 1.77 GeV.

Differential cross section for the W range 1.77 to 1.78 GeV.

Differential cross section for the W range 1.78 to 1.79 GeV.

Differential cross section for the W range 1.79 to 1.80 GeV.

Differential cross section for the W range 1.80 to 1.81 GeV.

Differential cross section for the W range 1.81 to 1.82 GeV.

Differential cross section for the W range 1.82 to 1.83 GeV.

Differential cross section for the W range 1.83 to 1.84 GeV.

Differential cross section for the W range 1.84 to 1.85 GeV.

Differential cross section for the W range 1.85 to 1.86 GeV.

Differential cross section for the W range 1.86 to 1.87 GeV.

Differential cross section for the W range 1.87 to 1.88 GeV.

Differential cross section for the W range 1.88 to 1.89 GeV.

Differential cross section for the W range 1.89 to 1.90 GeV.

Differential cross section for the W range 1.90 to 1.91 GeV.

Differential cross section for the W range 1.91 to 1.92 GeV.

Differential cross section for the W range 1.92 to 1.93 GeV.

Differential cross section for the W range 1.93 to 1.94 GeV.

Differential cross section for the W range 1.94 to 1.95 GeV.

Differential cross section for the W range 1.96 to 1.97 GeV.

Differential cross section for the W range 1.97 to 1.98 GeV.

Differential cross section for the W range 1.98 to 1.99 GeV.

Differential cross section for the W range 1.99 to 2.00 GeV.

Differential cross section for the W range 2.00 to 2.01 GeV.

Differential cross section for the W range 2.01 to 2.02 GeV.

Differential cross section for the W range 2.02 to 2.03 GeV.

Differential cross section for the W range 2.03 to 2.04 GeV.

Differential cross section for the W range 2.04 to 2.05 GeV.

Differential cross section for the W range 2.05 to 2.06 GeV.

Differential cross section for the W range 2.06 to 2.07 GeV.

Differential cross section for the W range 2.07 to 2.08 GeV.

Differential cross section for the W range 2.08 to 2.09 GeV.

Differential cross section for the W range 2.09 to 2.10 GeV.

Differential cross section for the W range 2.10 to 2.11 GeV.

Differential cross section for the W range 2.11 to 2.12 GeV.

Differential cross section for the W range 2.12 to 2.13 GeV.

Differential cross section for the W range 2.13 to 2.14 GeV.

Differential cross section for the W range 2.14 to 2.15 GeV.

Differential cross section for the W range 2.15 to 2.16 GeV.

Differential cross section for the W range 2.16 to 2.17 GeV.

Differential cross section for the W range 2.17 to 2.18 GeV.

Differential cross section for the W range 2.18 to 2.19 GeV.

Differential cross section for the W range 2.19 to 2.20 GeV.

Differential cross section for the W range 2.20 to 2.21 GeV.

Differential cross section for the W range 2.21 to 2.22 GeV.

Differential cross section for the W range 2.22 to 2.23 GeV.

Differential cross section for the W range 2.23 to 2.24 GeV.

Differential cross section for the W range 2.24 to 2.25 GeV.

Differential cross section for the W range 2.25 to 2.26 GeV.

Differential cross section for the W range 2.26 to 2.27 GeV.

Differential cross section for the W range 2.27 to 2.28 GeV.

Differential cross section for the W range 2.28 to 2.29 GeV.

Differential cross section for the W range 2.29 to 2.30 GeV.

Differential cross section for the W range 2.30 to 2.31 GeV.

Differential cross section for the W range 2.31 to 2.32 GeV.

Differential cross section for the W range 2.32 to 2.33 GeV.

Differential cross section for the W range 2.33 to 2.34 GeV.

Differential cross section for the W range 2.34 to 2.35 GeV.

Differential cross section for the W range 2.35 to 2.36 GeV.

Differential cross section for the W range 2.36 to 2.37 GeV.

Differential cross section for the W range 2.37 to 2.38 GeV.

Differential cross section for the W range 2.38 to 2.39 GeV.

Differential cross section for the W range 2.39 to 2.40 GeV.

Differential cross section for the W range 2.40 to 2.41 GeV.

Differential cross section for the W range 2.41 to 2.42 GeV.

Differential cross section for the W range 2.42 to 2.43 GeV.

Differential cross section for the W range 2.43 to 2.44 GeV.

Differential cross section for the W range 2.44 to 2.45 GeV.

Differential cross section for the W range 2.45 to 2.46 GeV.

Differential cross section for the W range 2.46 to 2.47 GeV.

Differential cross section for the W range 2.47 to 2.48 GeV.

Differential cross section for the W range 2.48 to 2.49 GeV.

Differential cross section for the W range 2.49 to 2.50 GeV.

Differential cross section for the W range 2.50 to 2.51 GeV.

Differential cross section for the W range 2.51 to 2.52 GeV.

Differential cross section for the W range 2.52 to 2.53 GeV.

Differential cross section for the W range 2.53 to 2.54 GeV.

Differential cross section for the W range 2.54 to 2.55 GeV.

Differential cross section for the W range 2.55 to 2.56 GeV.

Differential cross section for the W range 2.56 to 2.57 GeV.

Differential cross section for the W range 2.57 to 2.58 GeV.

Differential cross section for the W range 2.58 to 2.59 GeV.

Differential cross section for the W range 2.59 to 2.60 GeV.

Differential cross section for the W range 2.60 to 2.61 GeV.

Differential cross section for the W range 2.61 to 2.62 GeV.

Differential cross section for the W range 2.62 to 2.63 GeV.

Differential cross section for the W range 2.63 to 2.64 GeV.

Differential cross section for the W range 2.64 to 2.65 GeV.

Differential cross section for the W range 2.65 to 2.66 GeV.

Differential cross section for the W range 2.66 to 2.67 GeV.

Differential cross section for the W range 2.67 to 2.68 GeV.

Differential cross section for the W range 2.68 to 2.69 GeV.

Differential cross section for the W range 2.69 to 2.70 GeV.

Differential cross section for the W range 2.70 to 2.71 GeV.

Differential cross section for the W range 2.71 to 2.72 GeV.

Differential cross section for the W range 2.72 to 2.73 GeV.

Differential cross section for the W range 2.75 to 2.76 GeV.

Differential cross section for the W range 2.76 to 2.77 GeV.

Differential cross section for the W range 2.77 to 2.78 GeV.

Differential cross section for the W range 2.78 to 2.79 GeV.

Differential cross section for the W range 2.79 to 2.80 GeV.

Differential cross section for the W range 2.80 to 2.81 GeV.

Differential cross section for the W range 2.81 to 2.82 GeV.

Differential cross section for the W range 2.82 to 2.83 GeV.

Differential cross section for the W range 2.83 to 2.84 GeV.

Spin density matrix elements for the W range 1.72 to 1.73 GeV.

Spin density matrix elements for the W range 1.73 to 1.74 GeV.

Spin density matrix elements for the W range 1.74 to 1.75 GeV.

Spin density matrix elements for the W range 1.75 to 1.76 GeV.

Spin density matrix elements for the W range 1.76 to 1.77 GeV.

Spin density matrix elements for the W range 1.77 to 1.78 GeV.

Spin density matrix elements for the W range 1.78 to 1.79 GeV.

Spin density matrix elements for the W range 1.79 to 1.80 GeV.

Spin density matrix elements for the W range 1.80 to 1.81 GeV.

Spin density matrix elements for the W range 1.81 to 1.82 GeV.

Spin density matrix elements for the W range 1.82 to 1.83 GeV.

Spin density matrix elements for the W range 1.83 to 1.84 GeV.

Spin density matrix elements for the W range 1.84 to 1.85 GeV.

Spin density matrix elements for the W range 1.85 to 1.86 GeV.

Spin density matrix elements for the W range 1.86 to 1.87 GeV.

Spin density matrix elements for the W range 1.87 to 1.88 GeV.

Spin density matrix elements for the W range 1.88 to 1.89 GeV.

Spin density matrix elements for the W range 1.89 to 1.90 GeV.

Spin density matrix elements for the W range 1.90 to 1.91 GeV.

Spin density matrix elements for the W range 1.91 to 1.92 GeV.

Spin density matrix elements for the W range 1.92 to 1.93 GeV.

Spin density matrix elements for the W range 1.93 to 1.94 GeV.

Spin density matrix elements for the W range 1.94 to 1.95 GeV.

Spin density matrix elements for the W range 1.95 to 1.96 GeV.

Spin density matrix elements for the W range 1.96 to 1.97 GeV.

Spin density matrix elements for the W range 1.97 to 1.98 GeV.

Spin density matrix elements for the W range 1.98 to 1.99 GeV.

Spin density matrix elements for the W range 1.99 to 2.00 GeV.

Spin density matrix elements for the W range 2.00 to 2.01 GeV.

Spin density matrix elements for the W range 2.01 to 2.02 GeV.

Spin density matrix elements for the W range 2.02 to 2.03 GeV.

Spin density matrix elements for the W range 2.03 to 2.04 GeV.

Spin density matrix elements for the W range 2.04 to 2.05 GeV.

Spin density matrix elements for the W range 2.05 to 2.06 GeV.

Spin density matrix elements for the W range 2.06 to 2.07 GeV.

Spin density matrix elements for the W range 2.07 to 2.08 GeV.

Spin density matrix elements for the W range 2.08 to 2.09 GeV.

Spin density matrix elements for the W range 2.09 to 2.10 GeV.

Spin density matrix elements for the W range 2.10 to 2.11 GeV.

Spin density matrix elements for the W range 2.11 to 2.12 GeV.

Spin density matrix elements for the W range 2.12 to 2.13 GeV.

Spin density matrix elements for the W range 2.13 to 2.14 GeV.

Spin density matrix elements for the W range 2.14 to 2.15 GeV.

Spin density matrix elements for the W range 2.15 to 2.16 GeV.

Spin density matrix elements for the W range 2.16 to 2.17 GeV.

Spin density matrix elements for the W range 2.17 to 2.18 GeV.

Spin density matrix elements for the W range 2.18 to 2.19 GeV.

Spin density matrix elements for the W range 2.19 to 2.20 GeV.

Spin density matrix elements for the W range 2.20 to 2.21 GeV.

Spin density matrix elements for the W range 2.21 to 2.22 GeV.

Spin density matrix elements for the W range 2.22 to 2.23 GeV.

Spin density matrix elements for the W range 2.23 to 2.24 GeV.

Spin density matrix elements for the W range 2.24 to 2.25 GeV.

Spin density matrix elements for the W range 2.25 to 2.26 GeV.

Spin density matrix elements for the W range 2.26 to 2.27 GeV.

Spin density matrix elements for the W range 2.27 to 2.28 GeV.

Spin density matrix elements for the W range 2.28 to 2.29 GeV.

Spin density matrix elements for the W range 2.29 to 2.30 GeV.

Spin density matrix elements for the W range 2.30 to 2.31 GeV.

Spin density matrix elements for the W range 2.31 to 2.32 GeV.

Spin density matrix elements for the W range 2.32 to 2.33 GeV.

Spin density matrix elements for the W range 2.33 to 2.34 GeV.

Spin density matrix elements for the W range 2.34 to 2.35 GeV.

Spin density matrix elements for the W range 2.35 to 2.36 GeV.

Spin density matrix elements for the W range 2.36 to 2.37 GeV.

Spin density matrix elements for the W range 2.37 to 2.38 GeV.

Spin density matrix elements for the W range 2.38 to 2.39 GeV.

Spin density matrix elements for the W range 2.39 to 2.40 GeV.

Spin density matrix elements for the W range 2.40 to 2.41 GeV.

Spin density matrix elements for the W range 2.41 to 2.42 GeV.

Spin density matrix elements for the W range 2.42 to 2.43 GeV.

Spin density matrix elements for the W range 2.43 to 2.44 GeV.

Spin density matrix elements for the W range 2.44 to 2.45 GeV.

Spin density matrix elements for the W range 2.45 to 2.46 GeV.

Spin density matrix elements for the W range 2.46 to 2.47 GeV.

Spin density matrix elements for the W range 2.47 to 2.48 GeV.

Spin density matrix elements for the W range 2.48 to 2.49 GeV.

Spin density matrix elements for the W range 2.49 to 2.50 GeV.

Spin density matrix elements for the W range 2.50 to 2.51 GeV.

Spin density matrix elements for the W range 2.51 to 2.52 GeV.

Spin density matrix elements for the W range 2.52 to 2.53 GeV.

Spin density matrix elements for the W range 2.53 to 2.54 GeV.

Spin density matrix elements for the W range 2.54 to 2.55 GeV.

Spin density matrix elements for the W range 2.55 to 2.56 GeV.

Spin density matrix elements for the W range 2.56 to 2.57 GeV.

Spin density matrix elements for the W range 2.57 to 2.58 GeV.

Spin density matrix elements for the W range 2.58 to 2.59 GeV.

Spin density matrix elements for the W range 2.59 to 2.60 GeV.

Spin density matrix elements for the W range 2.60 to 2.61 GeV.

Spin density matrix elements for the W range 2.61 to 2.62 GeV.

Spin density matrix elements for the W range 2.62 to 2.63 GeV.

Spin density matrix elements for the W range 2.63 to 2.64 GeV.

Spin density matrix elements for the W range 2.64 to 2.65 GeV.

Spin density matrix elements for the W range 2.65 to 2.66 GeV.

Spin density matrix elements for the W range 2.66 to 2.67 GeV.

Spin density matrix elements for the W range 2.67 to 2.68 GeV.

Spin density matrix elements for the W range 2.68 to 2.69 GeV.

Spin density matrix elements for the W range 2.69 to 2.70 GeV.

Spin density matrix elements for the W range 2.70 to 2.71 GeV.

Spin density matrix elements for the W range 2.71 to 2.72 GeV.

Spin density matrix elements for the W range 2.72 to 2.73 GeV.

Spin density matrix elements for the W range 2.73 to 2.74 GeV.

Spin density matrix elements for the W range 2.74 to 2.75 GeV.

Spin density matrix elements for the W range 2.75 to 2.76 GeV.

Spin density matrix elements for the W range 2.76 to 2.77 GeV.

Spin density matrix elements for the W range 2.77 to 2.78 GeV.

Spin density matrix elements for the W range 2.78 to 2.79 GeV.

Spin density matrix elements for the W range 2.79 to 2.80 GeV.

Spin density matrix elements for the W range 2.80 to 2.81 GeV.

Spin density matrix elements for the W range 2.81 to 2.82 GeV.

Spin density matrix elements for the W range 2.82 to 2.83 GeV.

Spin density matrix elements for the W range 2.83 to 2.84 GeV.

Moments YLM(LM=00) of the di-pion angular distribution for -T.

Moments YLM(LM=00) of the di-pion angular distribution for -T.

Moments YLM(LM=00) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=10) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=11) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=20) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=21) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=22) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=30) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=31) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=32) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=33) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=40) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=41) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=42) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=43) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

Moments YLM(LM=44) of the di-pion angular distribution for -T.

S wave cross section for -T.

S wave cross section for -T.

S wave cross section for -T.

S wave cross section for -T.

S wave cross section for -T.

S wave cross section for -T.

P wave cross section for -T.

P wave cross section for -T.

P wave cross section for -T.

P wave cross section for -T.

P wave cross section for -T.

P wave cross section for -T.

Pm wave cross section for -T.

Pm wave cross section for -T.

Pm wave cross section for -T.

Pm wave cross section for -T.

Pm wave cross section for -T.

Pm wave cross section for -T.

P0 wave cross section for -T.

P0 wave cross section for -T.

P0 wave cross section for -T.

P0 wave cross section for -T.

P0 wave cross section for -T.

P0 wave cross section for -T.

Pp wave cross section for -T.

Pp wave cross section for -T.

Pp wave cross section for -T.

Pp wave cross section for -T.

Pp wave cross section for -T.

Pp wave cross section for -T.

D wave cross section for -T.

D wave cross section for -T.

D wave cross section for -T.

D wave cross section for -T.

D wave cross section for -T.

D wave cross section for -T.

Dm wave cross section for -T.

Dm wave cross section for -T.

Dm wave cross section for -T.

Dm wave cross section for -T.

Dm wave cross section for -T.

Dm wave cross section for -T.

D0 wave cross section for -T.

D0 wave cross section for -T.

D0 wave cross section for -T.

D0 wave cross section for -T.

D0 wave cross section for -T.

D0 wave cross section for -T.

Dp wave cross section for -T.

Dp wave cross section for -T.

Dp wave cross section for -T.

Dp wave cross section for -T.

Dp wave cross section for -T.

Dp wave cross section for -T.

F wave cross section for -T.

F wave cross section for -T.

F wave cross section for -T.

F wave cross section for -T.

F wave cross section for -T.

F wave cross section for -T.

Fm wave cross section for -T.

Fm wave cross section for -T.

Fm wave cross section for -T.

Fm wave cross section for -T.

Fm wave cross section for -T.

Fm wave cross section for -T.

F0 wave cross section for -T.

F0 wave cross section for -T.

F0 wave cross section for -T.

F0 wave cross section for -T.

F0 wave cross section for -T.

F0 wave cross section for -T.

Fp wave cross section for -T.

Fp wave cross section for -T.

Fp wave cross section for -T.

Fp wave cross section for -T.

Fp wave cross section for -T.

Fp wave cross section for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the P-wave for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Spin density matrix elements for the interference between the S- and P-waves for -T.

Mean value of the event shape variable C-PARAM.

Mean value of the event shape variable 1-THRUST(C=G).

Mean value of the event shape variable B(C=G).

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape RHO**2 corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape C-PARAM corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape THRUST(C=T) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape B(C=T) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape THRUST(C=G) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape B(C=G) corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

Differential distribution for event shape Y2 corrected to the hadron level for the Q**2 range 10240 TO 20480 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 80 TO 160 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 160 TO 320 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 320 TO 640 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 640 TO 1280 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 1280 TO 2560 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 2560 TO 5120 GeV**2.

Differential distribution for event shape (KOUT/Q) corrected to the hadron level for the Q**2 range 5120 TO 10240 GeV**2.

The measured differential jet shape.

The measured differential jet shape.

The measured differential jet shape.

The measured integrated jet shape.

The measured integrated jet shape.

The measured integrated jet shape.

The measured integrated jet shape.

The measured integrated jet shape.

The measured integrated jet shape.

The measured integrated cross section for R = 0.3 as a function of the meanPT.

Exclusive GAMMA* P --> PHI P cross section in the Q**2 range 9 to 30 GeV**2.

Parameter of the fit SIG of the form W**POWER as a function of Q**2.

Exclusive GAMMA* P --> PHI P cross section as a function of Q**2 for W=75 GeV.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=2.4 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=3.6 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=5.2 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=6.9 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=9.2 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=12.6 GeV**2.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV at Q**2=19.7 GeV**2.

The slope parameter and DSIG/DT at T=0 for the exclusive reaction GAMMA* P --> PHI P at W=75 GeV.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P as a function of W at Q**2=5 GeV**2 and ABS(T) = 0.73 GeV**2.. Error is combined statistics and systematics.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P as a function of W at Q**2=5 GeV**2 and ABS(T) = 0.45 GeV**2.. Error is combined statistics and systematics.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P as a function of W at Q**2=5 GeV**2 and ABS(T) = 0.25 GeV**2.. Error is combined statistics and systematics.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P as a function of W at Q**2=5 GeV**2 and ABS(T) = 0.12 GeV**2.. Error is combined statistics and systematics.

Differential DSIG/DT distribution for the exclusive reaction GAMMA* P --> PHI P as a function of W at Q**2=5 GeV**2 and ABS(T) = 0.025 GeV**2.. Error is combined statistics and systematics.

The parameter of the fit SIG of the form W**POWER as a function of T. From this the pomeron trajectory can be calculated a(1+POWER/4).

The spin density matrix element R04_00 and ratios of longitudinal and transversely polarized photons as a function of Q**2.

The spin density matrix element R04_00 and ratios of longitudinal and transversely polarized photons as a function of W for the Q**2 region 2 to 5 GeV**2.

The spin density matrix element R04_00 and ratios of longitudinal and transversely polarized photons as a function of W for the Q**2 region 5 to 20 GeV**2.

The luminosity weighted average polarized differential cross sections. The data are averaged over the eight centre of mass energies and over the COS(THETA(W)) bin width.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=+-) etc. see the text of the paper.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=+0) etc. see the text of the paper.

The luminosity weighted average CP-odd and CPThat-odd observables. For definition of SIG(C=-0) etc. see the text of the paper.

Mean value of the event shape variables C-PARAM in different Q**2 and X bins.

Mean value of the event shape variables 1-THRUST(C=G) in different Q**2 and X bins.

Mean value of the event shape variables B(C=G) in different Q**2 and X bins.