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\@writefile{lof}{\contentsline {figure}{\numberline {25}{\ignorespaces  Structure function $F_2^{\gamma Z}$ for data (solid points) and the expectation from H1PDF\tmspace  +\thinmuskip {.1667em}2012 (solid curve). The measurement at $Q^2=30\tmspace  +\thinmuskip {.1667em}000\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$ is now shown. The inner error bars represent the statistical uncertainties and the full error bar corresponds to the total measurement uncertainty. }}{119}{figure.25}}
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\@writefile{lof}{\contentsline {figure}{\numberline {26}{\ignorespaces  Structure function $F_2^{\gamma Z}$ transformed to $Q^2=1\tmspace  +\thinmuskip {.1667em}500\tmspace  +\thinmuskip {.1667em}{\rm  GeV}^2$ for data (solid points) and the expectation from H1PDF\tmspace  +\thinmuskip {.1667em}2012 (solid curve). The inner error bars represent the statistical uncertainties and the full error bar corresponds to the total measurement uncertainty.}}{120}{figure.26}}
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\@writefile{lof}{\contentsline {figure}{\numberline {27}{\ignorespaces  Structure function $xF_3^{\gamma Z}$ for the combined HERA\tmspace  +\thinmuskip {.1667em}I+II data (solid points) and the expectation from H1PDF\tmspace  +\thinmuskip {.1667em}2012 (solid curve). The inner error bars represent the statistical uncertainties and the full error bar corresponds to the total measurement uncertainty.}}{121}{figure.27}}
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\@writefile{lof}{\contentsline {figure}{\numberline {28}{\ignorespaces  Structure function $xF_3^{\gamma Z}$ transformed to $Q^2=1\tmspace  +\thinmuskip {.1667em}500$\tmspace  +\thinmuskip {.1667em}GeV$^2$ for data (solid points) and the expectation from H1PDF\tmspace  +\thinmuskip {.1667em}2012 (solid curve). The inner error bars represent the statistical uncertainties and the full error bar corresponds to the total measurement uncertainty.}}{122}{figure.28}}
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\@writefile{lof}{\contentsline {figure}{\numberline {29}{\ignorespaces  Dependence of the $e^\pm p$ CC cross sections on the longitudinal lepton beam polarisation $P_e$. The inner and outer error bars represent the statistical and total errors respectively. The uncertainties on the polarisation measurement are shown with horizontal error bars which are mostly smaller than the symbol size. The data are compared to the Standard Model expectation based on the H1PDF\tmspace  +\thinmuskip {.1667em}2012 parametrisation (dark shaded band). The light shaded band corresponds to the resulting one standard deviation contour of a linear fit to the data shown as the central line.}}{123}{figure.29}}
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