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\@writefile{lot}{\contentsline {table}{\numberline {1}{\ignorespaces  The DVCS cross section $\gamma ^\ast p \rightarrow \gamma p$, $\sigma _{DVCS}$, as a function of $Q^2$ for $W=82\tmspace  +\thinmuskip {.1667em}{\rm  GeV}$ and as a function of $W$ for $Q^2=10\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$, both for $ |t| < 1\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$. The first errors are statistical, the second systematic.}}{15}}
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\@writefile{lot}{\contentsline {table}{\numberline {2}{\ignorespaces The DVCS cross section $\gamma ^\ast p \rightarrow \gamma p$, $\sigma _{DVCS}$, as a function of $W$ for three $Q^2$ values and for $ |t| < 1\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$. The values of $\delta (Q^2)$ obtained from fits of the form $W^\delta $ are given. The first errors are statistical, the second systematic.}}{15}}
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\@writefile{lot}{\contentsline {table}{\numberline {3}{\ignorespaces  The DVCS cross section $\gamma ^* p\rightarrow \gamma p$, differential in $t$, $d\sigma _{DVCS}/dt$, for three values of $Q^2$ at $W=82\tmspace  +\thinmuskip {.1667em}{\rm  GeV}$, and for three values of $W$ at $Q^2=10\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$. Results for the corresponding $t$-slope parameters $b$ are given. The first errors are statistical, the second systematic.}}{16}}
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\@writefile{lot}{\contentsline {table}{\numberline {4}{\ignorespaces  The DVCS beam charge asymmetry $A_C(\phi )$ as a function of $\phi $ and integrated over the kinematic range $6.5 < Q^2 < 80\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$, $30 < W < 140\tmspace  +\thinmuskip {.1667em}{\rm  GeV}$ and $|t| < 1\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$. The first errors are statistical, the second systematic.}}{16}}
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\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces  Distributions of the energy (a) and polar angle (b) of the scattered electron, the energy (c) and polar angle (d) of the photon, the $\phi $ azimuthal angle between the plane of incoming and outgoing lepton and the plane of virtual and real photon\nobreakspace  {}\cite  {bel} (e) and the proton four momentum transfer squared $|t|$ (f). The data correspond to the full $e^{\pm }p$ sample and are compared to Monte Carlo expectations for elastic DVCS, elastic and inelastic BH and inelastic DVCS. All Monte Carlo simulations are normalised according to the luminosity of the data. The open histogram shows the total prediction and the shaded band its estimated uncertainty. }}{17}}
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\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces  The DVCS cross section $\gamma ^\ast p \rightarrow \gamma p$ as a function of $Q^2$ at $W=82$\nobreakspace  {}GeV (a) and as a function of $W$ at $Q^2=10$\nobreakspace  {}GeV$^2$ (b). The results from the previous H1\nobreakspace  {}\cite  {dvcsh1a} and ZEUS\nobreakspace  {}\cite  {dvcszeusb} publications based on HERA\nobreakspace  {}I data are also displayed. ZEUS measurements are propagated from $W=104$\nobreakspace  {}GeV to $82$\nobreakspace  {}GeV using a $W$ dependence $W^{0.52}$. The inner error bars represent the statistical errors, the outer error bars the statistical and systematic errors added in quadrature. The dashed line represents the prediction of the GPD model\nobreakspace  {}{\cite  {muller}} and the solid line the prediction of the dipole model\nobreakspace  {}{\cite  {gregory}}. }}{18}}
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\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces  The DVCS cross section $\gamma ^\ast p \rightarrow \gamma p$ as a function of $W$ at three values of $Q^2$ (a). The solid lines represent the results of fits of the form $W^\delta $. The fitted values of $\delta (Q^2)$ are shown in (b) together with the values obtained using HERA I data\nobreakspace  {}{\cite  {dvcsh1a}}. The inner error bars represent the statistical errors, the outer error bars the statistical and systematic errors added in quadrature. }}{19}}
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\@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces  The fitted $t$-slope parameters $b(Q^2)$ are shown in (a) together with the $t$-slope parameters from the previous H1\nobreakspace  {}\cite  {dvcsh1a} and ZEUS\nobreakspace  {}\cite  {dvcszeusb} publications based on HERA I data. In (b) the fitted $t$-slope parameters $b(W)$ are shown. The inner error bars represent the statistical errors and the outer error bars the statistical and systematic errors added in quadrature. The dashed line represents the prediction of the GPD model\nobreakspace  {}{\cite  {muller}} and the solid line the prediction of the dipole model\nobreakspace  {}{\cite  {gregory}}. }}{20}}
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\@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces  The inelastic DVCS cross section differential in $t$ at $W=82$\nobreakspace  {}GeV and $Q^2=10$\nobreakspace  {}GeV$^2$ and for events with $1.4 \lesssim M_Y \lesssim 10$\nobreakspace  {}GeV. The inner error bars represent the statistical errors, the outer error bars the statistical and systematic errors added in quadrature. }}{20}}
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\@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces  Beam charge asymmetry as a function of the angle $\phi $ as defined in\nobreakspace  {}\cite  {bel}, integrated over the kinematic range of the analysis. The inner error bars represent the statistical errors, the outer error bars the statistical and systematic errors added in quadrature. The function $0.16 \qopname  \relax o{cos}\phi $ is also shown (solid line), together with the GPD model prediction (dashed line). }}{21}}
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