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\contentsline {table}{\numberline {1.1}{\ignorespaces Properties of Left-Handed Fermions}}{5}{table.1.1}
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\contentsline {table}{\numberline {8.1}{\ignorespaces Integrated polarized inclusive-jet cross-sections $\sigma _{\rm jets}$ for jets of hadrons in the laboratory frame selected with the longitudinally invariant $k_{T}$ cluster algorithm, described in section\nobreakspace {}\ref {section_jet_reconstruction}. The statistical, uncorrelated systematic and energy-scale ({\rm ES}) uncertainties are shown separately. The uncertainty coming from the luminosity measurement is not listed. The predictions of the SM as given by the {\textsc {Mepjet}} calculations and are shown in the last column.}}{96}{table.8.1}
\contentsline {table}{\numberline {8.2}{\ignorespaces Integrated unpolarized jet cross-sections $\sigma _{\rm jets}$ for jets of hadrons in the laboratory frame selected with the longitudinally invariant $k_{T}$ cluster algorithm. The statistical, uncorrelated systematic and energy-scale ({\rm ES}) uncertainties are shown separately. The predictions of QCD as given by the {\textsc {Mepjet}} calculations using the ZEUS-S PDFs are shown at NLO for the inclusive-jet and dijet cross sections and at LO for the three-jet cross sections, together with the total theoretical uncertainty. Also shown are the total cross sections predicted by QCD using the CTEQ6 or MRST PDF sets.}}{101}{table.8.2}
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\contentsline {table}{\numberline {E.1}{\ignorespaces First Level Trigger Bits Applied}}{136}{table.E.1}
\contentsline {table}{\numberline {E.2}{\ignorespaces EXO4 Second Level Trigger Definitions}}{138}{table.E.2}
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\contentsline {table}{\numberline {G.1}{\ignorespaces Differential polarized inclusive-jet cross-sections $d\sigma /d\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ for jets of hadrons in the laboratory frame selected with the longitudinally invariant $k_{T}$ cluster algorithm. The statistical, uncorrelated systematic and energy-scale ({\rm ES}) uncertainties are shown separately.}}{146}{table.G.1}
\contentsline {table}{\numberline {G.2}{\ignorespaces Differential polarized inclusive-jet cross-sections $d\sigma /dE_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$. Other details as in the caption to Table\nobreakspace {}\ref {table_rap_xs_pol}.}}{147}{table.G.2}
\contentsline {table}{\numberline {G.3}{\ignorespaces Differential polarized inclusive-jet cross-sections $d\sigma /dQ^2$. Other details as in the caption to Table\nobreakspace {}\ref {table_rap_xs_pol}.}}{148}{table.G.3}
\contentsline {table}{\numberline {G.4}{\ignorespaces Differential polarized inclusive-jet cross-sections $d\sigma /dx$. Other details as in the caption to Table\nobreakspace {}\ref {table_rap_xs_pol}.}}{149}{table.G.4}
\contentsline {table}{\numberline {G.5}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /d\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ and $d\sigma /d\overline {\eta }^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ in $e^-p$ collisions for jets of hadrons in the laboratory frame selected with the longitudinally invariant $k_{T}$ cluster algorithm. The statistical, uncorrelated systematic and jet-energy-scale ({\rm ES}) uncertainties are shown separately. The multiplicative corrections for QED radiative effects, $C_{\rm QED}$, and the corrections for hadronization effects, $C_{\rm had}$, to be applied to the parton-level NLO QCD calculations, are shown in the last two columns.}}{150}{table.G.5}
\contentsline {table}{\numberline {G.6}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /d\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ and $d\sigma /\overline {\eta }^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ in $e^+p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{151}{table.G.6}
\contentsline {table}{\numberline {G.7}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /dE_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ and $d\sigma /d\overline {E}_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ in $e^-p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{152}{table.G.7}
\contentsline {table}{\numberline {G.8}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /dE_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ and $d\sigma /d\overline {E}_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ in $e^+p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{153}{table.G.8}
\contentsline {table}{\numberline {G.9}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /dQ^2$ in $e^-p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{154}{table.G.9}
\contentsline {table}{\numberline {G.10}{\ignorespaces Differential unpolarized inclusive-jet, dijet and three-jet cross-sections $d\sigma /dQ^2$ in $e^+p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{155}{table.G.10}
\contentsline {table}{\numberline {G.11}{\ignorespaces Differential unpolarized inclusive-jet cross-sections $d\sigma /dx$ in $e^-p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{156}{table.G.11}
\contentsline {table}{\numberline {G.12}{\ignorespaces Differential unpolarized inclusive-jet cross-sections $d\sigma /dx$ in $e^+p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{156}{table.G.12}
\contentsline {table}{\numberline {G.13}{\ignorespaces Differential unpolarized dijet and three-jet cross-sections $d\sigma /dm^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jj}}$ and $d\sigma /dm^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jj}}$ in $e^-p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{157}{table.G.13}
\contentsline {table}{\numberline {G.14}{\ignorespaces Differential unpolarized dijet and three-jet cross-sections $d\sigma /dm^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jj}}$ and $d\sigma /dm^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont 3j}}$ in $e^+p$ collisions. Other details as in the caption to Table\nobreakspace {}\ref {table_upol_rapjet_e}.}}{158}{table.G.14}
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