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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

ENERGY DEPENDENCE OF DENSITY MATRIX ELEMENTS.

No description provided.

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 $|y| < 1$.

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, $110 < N_\text{ch} \le 140$.

Spin alignment RHO(00) extracted from the helicity angle distributions for PHI and OMEGA production in the given XF regions for different M(PV) regions. The uncertainty is the propagated uncertainty from the linear fits, which in turn includes the quadratic sum of statistical uncertainties and uncertainties from the background subtraction.

Spin alignment RHO(00) extracted using DELTA(P), the direction of the momentum transfer from the beam proton in the initial state to the fast proton in the final state, as the reference axis. The table includes PHI and OMEGA production. The results for different P(V) cuts are also given for OMEGA production. The uncertainty is the propagated uncertainty from the linear fits, which in turn includes the quadratic sum of statistical uncertainties and uncertainties from the background subtraction.

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.

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.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA P --> PHI P reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA P --> PHI P reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA P --> PHI P reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI P N reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI P N reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI P N reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI DEUT reaction in the helicity system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI DEUT reaction in the Gottfried-Jackson system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=0,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=0,MM=11) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=00) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RE(RHO(JJ=1,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element RHO(JJ=1,MM=1-1) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=10)) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Measurements of the spin density matrix element IM(RHO(JJ=2,MM=1-1)) for the GAMMA DEUT --> PHI DEUT reaction in the Adair system as a function of T-Tmin for 3 incident photon energy regions.

Q**2 dependence of the GAMMA* P cross section for proton dissociative PHI meson production at mean W There is an additional overall normalization uncertainty of 5.3 PCT.

Q**2 dependence of the ratio pf the PHI to RHO0 elastic cross section for mean W There is an additional overall normalization uncertainty of 4.0 PCT.

Q**2 + MASS(V)**2 dependence of the ratio pf the PHI to RHO0 elastic cross section for mean W There is an additional overall normalization uncertainty of 4.0 PCT.

Q**2 dependence of the longitudinal and transverse GAMMA* P cross sections for elastic RHO0 production at mean W There is an additional overall normalization uncertainty of 3.9 PCT.

Q**2 dependence of the longitudinal and transverse GAMMA* P cross sections for elastic PHI production at mean W There is an additional overall normalization uncertainty of 4.7 PCT.

W dependence of the GAMMA* P cross section for elastic RHO0 production for Q**2 There is an additional overall normalization uncertainty of 3.9 PCT.

W dependence of the GAMMA* P cross section for elastic RHO0 production for Q**2 There is an additional overall normalization uncertainty of 3.9 PCT.

W dependence of the GAMMA* P cross section for elastic RHO0 production for Q**2 There is an additional overall normalization uncertainty of 3.9 PCT.

W dependence of the GAMMA* P cross section for elastic RHO0 production for Q**2 There is an additional overall normalization uncertainty of 3.9 PCT.

W dependence of the GAMMA* P cross section for elastic RHO0 production for Q**2 There is an additional overall normalization uncertainty of 3.9 PCT.

W dependence of the GAMMA* P cross section for dissociative RHO0 production for Q**2 There is an additional overall normalization uncertainty of 4.6 PCT.

W dependence of the GAMMA* P cross section for dissociative RHO0 production for Q**2 There is an additional overall normalization uncertainty of 4.6 PCT.

W dependence of the GAMMA* P cross section for dissociative RHO0 production for Q**2 There is an additional overall normalization uncertainty of 4.6 PCT.

W dependence of the GAMMA* P cross section for elastic PHI production for Q**2 There is an additional overall normalization uncertainty of 4.7 PCT.

W dependence of the GAMMA* P cross section for elastic PHI production for Q**2 There is an additional overall normalization uncertainty of 4.7 PCT.

W dependence of the GAMMA* P cross section for elastic PHI production for Q**2 There is an additional overall normalization uncertainty of 4.7 PCT.

W dependence of the GAMMA* P cross section for dissociative PHI production for Q**2 There is an additional overall normalization uncertainty of 5.3 PCT.

T dependence of the GAMMA* P cross section for elastic RHO0 production for several values. There is an additional overall normalization uncertainty of 3.9 PCT.

T dependence of the GAMMA* P cross section for dissociative RHO0 production for several values. There is an additional overall normalization uncertainty of 4.6 PCT.

T dependence of the GAMMA* P cross section for elastic PHI production for several values. There is an additional overall normalization uncertainty of 4.7 PCT.

T dependence of the GAMMA* P cross section for dissociative PHI production for several values. There is an additional overall normalization uncertainty of 5.3 PCT.

Q**2 dependence of the slope of the T distribution in elastic RHO0 production.

Q**2 dependence of the slope of the T distribution in elastic PHI production.

Q**2 dependence of the slope of the T distribution in dissociative RHO0 production.

Q**2 dependence of the slope of the T distribution in dissociative PHI production.

W dependence of the GAMMA* P cross section for dissociative RHO0 production in four ABS(T) bins at Q**2 There is an additional normalization uncertainty of 4 PCT.

W dependence of the GAMMA* P cross section for dissociative RHO0 production in four ABS(T) bins at Q**2 There is an additional normalization uncertainty of 4 PCT.

Q**2 dependence of the ratio of proton dissociative to elastic RHO0 meson total cross section. There is an additional overall normalization uncertainty of 2.4 PCT.

Q**2 dependence of the ratio of proton dissociative to elastic PHI meson total cross section. There is an additional overall normalization uncertainty of 2.4 PCT.

Q**2 dependence of the ratio of proton dissociative to elastic RHO0 meson differential cross section at T=0. There is an additional overall normalization uncertainty of 2.4 PCT.

Q**2 dependence of the ratio of proton dissociative to elastic PHI mesondifferential cross section at T=0. There is an additional overall normalization uncertainty of 2.4 PCT.

Slope differences between elastic and proton dissociative scattering for RHO0 meson production.

Slope differences between elastic and proton dissociative scattering for PHI meson production.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of Q**2.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of W.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of PHI mesons as a function of T.

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Spin density matrix elements for diffractive electroproduction of RHO0 mesons as a function of M(PI+PI-).

Q**2 dependence of the matrix element combination RHO(JJ=5,MM=00) + 2*RHO(JJ=5,MM=11).

Q**2 dependence of the matrix element combination RHO(JJ=1,MM=00) + 2*RHO(JJ=1,MM=11).

T dependence of the matrix element combination RHO(JJ=5,MM=00) + 2*RHO(JJ=5,MM=11).

T dependence of the matrix element combination RHO(JJ=1,MM=00) + 2*RHO(JJ=1,MM=11).

Q**2 dependence of the ratio R.

Q**2 dependence of the ratio R.

W dependence of the ratio R.

W dependence of the ratio R.

W dependence of the ratio R.

T dependence of the ratio R.

T dependence of the ratio R.

Di-pion mass dependence of the ratio R.

Di-pion mass dependence of the ratio R.

Dependence of the exponential slope of the T distribution as a function of the di-pion mass for the Q**2 range 2.5 to 5 GeV**2.

Dependence of the exponential slope of the T distribution as a function of the di-pion mass for the Q**2 range 5 to 60 GeV**2.

Q**2 dependence of the ratio of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for RHO0 production.

Q**2 dependence of the ratio of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for PHI production.

T dependence of the ratio of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for RHO0 production in the Q**2 range 2.5 to 5 GeV**2.

T dependence of the ratio of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for RHO0 production in the Q**2 range 5 to 60 GeV**2.

T dependence of the ratio of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for PHI production in the Q**2 range 2.5 to 60 GeV**2.

Di-pion mass dependence of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for RHO0 production in the Q**2 range 2.5 to 5 GeV**2.

Di-pion mass dependence of the helicity amplitudes (assumed purely imaginary) and phase difference between the T11 and T00 amplitudes for RHO0 production in the Q**2 range 5 to 60 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 3.0 to 4.0 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 4.0 to 5.0 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 5.0 to 6.5 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 6.5 to 8.0 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 8.0 to 11.0 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 11.0 to 20.0 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 2 to 3 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 3 to 5 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 5 to 10 GeV**2.

The differential cross section DSIG/DT as a function of W in the ABS(T) range 10 to 20 GeV**2.

Spin density events as a function of T.

Differential cross section DSIG/DT for photon energy 1.87 to 1.97 GeV.

Differential cross section DSIG/DT for photon energy 1.97 to 2.07 GeV.

Differential cross section DSIG/DT for photon energy 2.07 to 2.17 GeV.

Differential cross section DSIG/DT for photon energy 2.17 to 2.27 GeV.

Differential cross section DSIG/DT for photon energy 2.27 to 2.37 GeV.

The fitted value of DSIG/DT at T=TMIN as a function of the photon energy.

DSIG/DT distribution over the full photon energy range with statistical errors only.

Mean decay asymmetry measured over the photon energy range 1.87 to 2.37 GeV.

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

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

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

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

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

The central region charged particle density.

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

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.

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the axis which maximises the sum of the longitudinal momenta in the current hemisphere, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of (1-THRUST) where THRUST is w.r.t the vitrual photon axis, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised distribution of the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Normalised distribution of the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Normalised distribution of the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Normalised distribution of the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Normalised distribution of the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Normalised distribution of the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Normalised distribution of the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Mean values of the event shape variables.

Covariance matrix for (1-THRUST(C)), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST(C)), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST(C)), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST(C)), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST(C)), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST(C)), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST(C)), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for (1-THRUST), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for (1-THRUST), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for (1-THRUST), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for (1-THRUST), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for (1-THRUST), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for (1-THRUST), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for (1-THRUST), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the Jet Broadening (B), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the Jet Broadening (B), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the Jet Broadening (B), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the Jet Broadening (B), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the Jet Broadening (B), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the Jet Broadening (B), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the Jet Broadening (B), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the squared Jet Mass (RHO), for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Covariance matrix for the C-Parameter, for Q = 14.0 to 16.0 GeV and X = 0.00841 .

Covariance matrix for the C-Parameter, for Q = 16.0 to 20.0 GeV and X = 0.01180 .

Covariance matrix for the C-Parameter, for Q = 20.0 to 30.0 GeV and X = 0.02090 .

Covariance matrix for the C-Parameter, for Q = 30.0 to 50.0 GeV and X = 0.04910 .

Covariance matrix for the C-Parameter, for Q = 50.0 to 70.0 GeV and X = 0.11600 .

Covariance matrix for the C-Parameter, for Q = 70.0 to 100.0 GeV and X = 0.19900 .

Covariance matrix for the C-Parameter, for Q = 100.0 to 200.0 GeV and X = 0.32300 .

Normalised decay angular distribution w.r.t. the azimuthal anlge PHI.

Spin density matrix elements from fot to the decay angular distributions.

Differential cross section as a function of T+ABS(TMIN) in the photon energy range 1.87 to 1.97 GeV.

Differential cross section as a function of T+ABS(TMIN) in the photon energy range 1.97 to 2.07 GeV.

Differential cross section as a function of T+ABS(TMIN) in the photon energy range 2.07 to 2.17 GeV.

Differential cross section as a function of T+ABS(TMIN) in the photon energy range 2.17 to 2.27 GeV.

Differential cross section as a function of T+ABS(TMIN) in the photon energy range 2.27 to 2.37 GeV.

Energy dependence of the measured values of DSIG/DT at -ABS(T(C=MIN)).

Values of RHO1 from fits to the measured angular distributions in the T+ABS(TMIN) range 0.20 to 0 GeV**2 in two energy regions.

Values of RHO2 from fits to the measured angular distributions in the T+ABS(TMIN) range 0.20 to 0 GeV**2 in two energy regions.

Values of RHO3 from fits to the measured angular distributions in the T+ABS(TMIN) range 0.20 to 0 GeV**2 in two energy regions.

Values of RHO4 from fits to the measured angular distributions in the T+ABS(TMIN) range 0.20 to 0 GeV**2 in two energy regions.

Values of RHO5 from fits to the measured angular distributions in the T+ABS(TMIN) range 0.20 to 0 GeV**2 in two energy regions.

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.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 172.3 GeV.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 182.8 GeV.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 188.6 GeV.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 194.4 GeV.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 200.2 GeV.

Jet fractions using the JADE algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 130.1 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 136.1 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 161.3 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 172.3 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 182.8 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 188.6 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 194.4 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 200.2 GeV.

Jet fractions using the KT(Durham) algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.

Jet fractions using the Cambridge algorithm as a function of the jet resolution parameter YCUT at c.m. energy 202.2 GeV.

Jet fractions using the Cambridge algorithm as a function of the jet resolution parameter YCUT at c.m. energy 206.2 GeV.

Differential distributions for event thrust.

Differential distributions for event thrust.

Differential distributions for event thrust.

Differential distributions for event thrust.

Differential distributions for event thrust.

Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).

Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).

Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).

Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).

Differential distributions for the scaled heavy jet mass (RHO(C=HEAVY)).

Differential distributions for total jet broadening (BT).

Differential distributions for total jet broadening (BT).

Differential distributions for total jet broadening (BT).

Differential distributions for total jet broadening (BT).

Differential distributions for total jet broadening (BT).

Differential distributions for wide jet broadening (BW).

Differential distributions for wide jet broadening (BW).

Differential distributions for wide jet broadening (BW).

Differential distributions for wide jet broadening (BW).

Differential distributions for wide jet broadening (BW).

Differential distributions for the C-Parameter.

Differential distributions for the C-Parameter.

Differential distributions for the C-Parameter.

Differential distributions for the D-Parameter.

Differential distributions for the D-Parameter.

Differential distributions for the D-Parameter.

Differential distributions for the THRUST at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.

Differential distributions for the RHO(C=HEAVY) at c.m. energy 91.2 GeV forlight quark (udsc) and b quark events.

Differential distributions for the BT at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.

Differential distributions for the BW at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.

Differential distributions for the C-PARAM at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.

Differential distributions for the D-PARAM at c.m. energy 91.2 GeV for light quark (udsc) and b quark events.

Mean values (first moment) and dispersion (second moment) of the THRUST distribution as a function of c.m. energy.

Mean values (first moment) and dispersion (second moment) of the scaled heavy jet mass (RHO(C=HEAVY)) as a function of c.m. energy.

Mean values (first moment) and dispersion (second moment) of the total jet broadening (BT) as a function of c.m. energy.

Mean values (first moment) and dispersion (second moment) of the wide jet broadening (BW) as a function of c.m. energy.

Mean values (first moment) and dispersion (second moment) of the C-PARAM as a function of c.m. energy.

Mean values (first moment) and dispersion (second moment) of the D-PARAM as a function of c.m. energy.

Charged particle multiplicities at c.m. energy 91.2 GeV for all flavour, light quark (udsc) and bottom (b) flavour events.

Charged particle multiplicity.

Charged particle multiplicity.

Charged particle multiplicity.

First and second moment of the charged particle multiplicity distribution at c.m. energy 91.2 GeV for all flavours and for udsc an b flavours.

First and second moment of the charged particle multiplicity distribution at c.m. energy.

Distribution of LN(1/X) at c.m. energy 91.2 GeV.

Distribution of LN(1/X) at higher c.m. energies.

Distribution of LN(1/X) at higher c.m. energies.

Distribution of LN(1/X) at higher c.m. energies.

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.