\addvspace {10\p@ }
\contentsline {figure}{\numberline {1.1}{\ignorespaces Behavior of the QED and QCD Couplings}}{9}{figure.1.1}
\contentsline {figure}{\numberline {1.2}{\ignorespaces L.O. Feynman Diagrams for NC and CC DIS}}{10}{figure.1.2}
\contentsline {figure}{\numberline {1.3}{\ignorespaces Schematic of LO jet Production in CC DIS}}{12}{figure.1.3}
\contentsline {figure}{\numberline {1.4}{\ignorespaces Schematic of BGF Dijet Production in CC DIS}}{13}{figure.1.4}
\contentsline {figure}{\numberline {1.5}{\ignorespaces A Diagram of The ZEUS Detector}}{15}{figure.1.5}
\contentsline {figure}{\numberline {1.6}{\ignorespaces Event Display Single Jet CC DIS}}{17}{figure.1.6}
\contentsline {figure}{\numberline {1.7}{\ignorespaces Event Display Dijet CC DIS}}{18}{figure.1.7}
\contentsline {figure}{\numberline {1.8}{\ignorespaces Event Display Dijet NC DIS}}{19}{figure.1.8}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {2.1}{\ignorespaces General Schematic of $ep$ Scattering}}{23}{figure.2.1}
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\contentsline {figure}{\numberline {3.1}{\ignorespaces Schematic Diagram of the DESY Accelerator Complex}}{32}{figure.3.1}
\contentsline {figure}{\numberline {3.2}{\ignorespaces A Diagram of The ZEUS CTD}}{37}{figure.3.2}
\contentsline {figure}{\numberline {3.3}{\ignorespaces Schematic of the ZEUS Calorimeter}}{40}{figure.3.3}
\contentsline {figure}{\numberline {3.4}{\ignorespaces Schematic of the ZEUS Luminosity System}}{42}{figure.3.4}
\contentsline {figure}{\numberline {3.5}{\ignorespaces Schematic of the ZEUS Trigger System}}{45}{figure.3.5}
\addvspace {10\p@ }
\addvspace {10\p@ }
\contentsline {figure}{\numberline {5.1}{\ignorespaces Schematic of MEPS}}{57}{figure.5.1}
\contentsline {figure}{\numberline {5.2}{\ignorespaces Schematic of CDM}}{58}{figure.5.2}
\contentsline {figure}{\numberline {5.3}{\ignorespaces Feynman Diagrams for Higher Order QED Effects}}{59}{figure.5.3}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {6.1}{\ignorespaces Schematic of CAL Timing Information}}{65}{figure.6.1}
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\contentsline {figure}{\numberline {7.1}{\ignorespaces Detector-Level Kinematic Variable Comparison between $e^{-}p$ Data and ARIADNE}}{77}{figure.7.1}
\contentsline {figure}{\numberline {7.2}{\ignorespaces Detector-Level Jet Variable Comparison between $e^{-}p$ Data and ARIADNE 1/2}}{78}{figure.7.2}
\contentsline {figure}{\numberline {7.3}{\ignorespaces Detector-Level Jet Variable Comparison between $e^{-}p$ Data and ARIADNE 2/2}}{79}{figure.7.3}
\contentsline {figure}{\numberline {7.4}{\ignorespaces Reconstruction of $P_{T}^{\relax \fontsize {10}{12}\selectfont \abovedisplayskip 10\p@ plus2\p@ minus5\p@ \abovedisplayshortskip \z@ plus3\p@ \belowdisplayshortskip 6\p@ plus3\p@ minus3\p@ \def \leftmargin \leftmargini \parsep 5\p@ plus2.5\p@ minus\p@ \topsep 10\p@ plus4\p@ minus6\p@ \itemsep 5\p@ plus2.5\p@ minus\p@ {\leftmargin \leftmargini \topsep 6\p@ plus2\p@ minus2\p@ \parsep 3\p@ plus2\p@ minus\p@ \itemsep \parsep }\belowdisplayskip \abovedisplayskip {\unhbox \voidb@x \hbox {miss}}}$}}{81}{figure.7.4}
\contentsline {figure}{\numberline {7.5}{\ignorespaces Reconstruction of $P_{T}^{\relax \fontsize {10}{12}\selectfont \abovedisplayskip 10\p@ plus2\p@ minus5\p@ \abovedisplayshortskip \z@ plus3\p@ \belowdisplayshortskip 6\p@ plus3\p@ minus3\p@ \def \leftmargin \leftmargini \parsep 5\p@ plus2.5\p@ minus\p@ \topsep 10\p@ plus4\p@ minus6\p@ \itemsep 5\p@ plus2.5\p@ minus\p@ {\leftmargin \leftmargini \topsep 6\p@ plus2\p@ minus2\p@ \parsep 3\p@ plus2\p@ minus\p@ \itemsep \parsep }\belowdisplayskip \abovedisplayskip {\unhbox \voidb@x \hbox {miss}}}$ and $y$}}{82}{figure.7.5}
\contentsline {figure}{\numberline {7.6}{\ignorespaces Reconstruction of $Q^2$}}{83}{figure.7.6}
\contentsline {figure}{\numberline {7.7}{\ignorespaces Reconstruction of $x$}}{84}{figure.7.7}
\contentsline {figure}{\numberline {7.8}{\ignorespaces Reconstruction of $E_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$}}{85}{figure.7.8}
\contentsline {figure}{\numberline {7.9}{\ignorespaces Reconstruction of $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$}}{86}{figure.7.9}
\contentsline {figure}{\numberline {7.10}{\ignorespaces Reconstruction of $\phi ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$}}{87}{figure.7.10}
\contentsline {figure}{\numberline {7.11}{\ignorespaces Jet Transverse Energy Before And After Corrections vs. $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$}}{88}{figure.7.11}
\contentsline {figure}{\numberline {7.12}{\ignorespaces Jet Transverse Energy Before And After Corrections vs. $\gamma _{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont H}}$}}{88}{figure.7.12}
\contentsline {figure}{\numberline {7.13}{\ignorespaces $E_T$ reconstruction vs. $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ and $\gamma _{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont H}}$}}{91}{figure.7.13}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {8.1}{\ignorespaces Polarized $e^-p$ and $e^+p$ $E_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Inclusive-Jet Cross sections}}{95}{figure.8.1}
\contentsline {figure}{\numberline {8.2}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Inclusive-Jet Cross sections}}{97}{figure.8.2}
\contentsline {figure}{\numberline {8.3}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $x$ Inclusive-Jet Cross sections}}{98}{figure.8.3}
\contentsline {figure}{\numberline {8.4}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $E_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Inclusive-Jet Cross sections}}{98}{figure.8.4}
\contentsline {figure}{\numberline {8.5}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $Q^2$ Inclusive-Jet Cross sections}}{99}{figure.8.5}
\contentsline {figure}{\numberline {8.6}{\ignorespaces \it Overview of theoretical uncertainties for the inclusive-jet cross sections in CC DIS for jets with $E_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}>14\nobreakspace {}{\unhbox \voidb@x \hbox {GeV}}$ and $-1<\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}<2.5$ in the kinematic regime given by $Q^2>200\nobreakspace {}{\unhbox \voidb@x \hbox {GeV}}^2$ and $y<0.9$ as functions of (a) $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$, (b) $E_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$, (c) $Q^2$ and (d) $x$ in $e^-p$ (shaded areas) and $e^+p$ (hatched areas) collisions. Shown are the relative uncertainties induced by the variation of the renormalization scale $\mu _{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont R}}$, the uncertainties on the proton PDFs and hadronization model. Also shown are the relative differences between the NLO QCD calculations using the CTEQ6 (dashed lines) or MRST (dot-dashed lines) PDF sets to the calculations based on the ZEUS sets. }}{102}{figure.8.6}
\contentsline {figure}{\numberline {8.7}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $\overline {\eta }^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ dijet cross sections}}{104}{figure.8.7}
\contentsline {figure}{\numberline {8.8}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $\overline {E}_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Dijet Cross sections}}{105}{figure.8.8}
\contentsline {figure}{\numberline {8.9}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $Q^2$ dijet cross sections}}{106}{figure.8.9}
\contentsline {figure}{\numberline {8.10}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $m^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jj}}$ Dijet Cross sections}}{107}{figure.8.10}
\contentsline {figure}{\numberline {8.11}{\ignorespaces Three-jet candidate event in CC DIS in the ZEUS detector. The event is viewed in the $x-y$ plane in (a), the $z-r$ view in (b), and $E_T$ of CAL deposition $\eta - \phi $ plane in (c). In (a) and (b), reconstructed tracks are superimposed over CTD hits, and CAL depositions are drawn proportional to the energy deposited. In (a), only the energy deposition in the barrel calorimeter is shown. In (a) an imbalance in the azimuthal distribution of tracks is observed. In (c), three broad CAL deposits are observed, which are separated in the $\eta - \phi $ plane. In (b), these are observed to penetrate into the second hadronic section of the CAL. These deposits were reconstructed as three jets. }}{108}{figure.8.11}
\contentsline {figure}{\numberline {8.12}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $\overline {\eta }^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Trijet Cross sections}}{109}{figure.8.12}
\contentsline {figure}{\numberline {8.13}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $\overline {E}_T^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Trijet Cross sections}}{110}{figure.8.13}
\contentsline {figure}{\numberline {8.14}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $Q^2$ Trijet Cross sections}}{111}{figure.8.14}
\contentsline {figure}{\numberline {8.15}{\ignorespaces Unpolarized $e^-p$ and $e^+p$ $m^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont 3j}}$ Trijet Cross sections}}{112}{figure.8.15}
\addvspace {10\p@ }
\addvspace {10\p@ }
\contentsline {figure}{\numberline {A.1}{\ignorespaces Detector-Level Kinematic Variable Comparison between $e^{+}p$ Data and ARIADNE}}{118}{figure.A.1}
\contentsline {figure}{\numberline {A.2}{\ignorespaces Detector-Level Jet Variable Comparison between $e^{+}p$ Data and ARIADNE 1/2}}{119}{figure.A.2}
\contentsline {figure}{\numberline {A.3}{\ignorespaces Detector-Level Jet Variable Comparison between $e^{+}p$ Data and ARIADNE 2/2}}{120}{figure.A.3}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {B.1}{\ignorespaces Monte Carlo Reweighting for the $e^{-}p$ Sample}}{122}{figure.B.1}
\contentsline {figure}{\numberline {B.2}{\ignorespaces Monte Carlo Reweighting for the $e^{+}p$ Sample}}{123}{figure.B.2}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {C.1}{\ignorespaces Inclusive Jet Purity, Efficiency, Acceptance $e^{-}p$ ARIADNE}}{125}{figure.C.1}
\contentsline {figure}{\numberline {C.2}{\ignorespaces Dijet Jet Purity, Efficiency, Acceptance $e^{-}p$ ARIADNE}}{126}{figure.C.2}
\contentsline {figure}{\numberline {C.3}{\ignorespaces Trijet Jet Purity, Efficiency, Acceptance $e^{-}p$ ARIADNE}}{127}{figure.C.3}
\addvspace {10\p@ }
\contentsline {figure}{\numberline {D.1}{\ignorespaces Inclusive Jet Theoretical Uncertainties $e^{-}p$ }}{129}{figure.D.1}
\contentsline {figure}{\numberline {D.2}{\ignorespaces Dijet Theoretical Uncertainties $e^{-}p$ }}{130}{figure.D.2}
\contentsline {figure}{\numberline {D.3}{\ignorespaces Trijet Theoretical Uncertainties $e^{-}p$ }}{131}{figure.D.3}
\contentsline {figure}{\numberline {D.4}{\ignorespaces Inclusive Jet Theoretical Uncertainties $e^{+}p$ }}{132}{figure.D.4}
\contentsline {figure}{\numberline {D.5}{\ignorespaces Dijet Theoretical Uncertainties $e^{+}p$ }}{133}{figure.D.5}
\contentsline {figure}{\numberline {D.6}{\ignorespaces Trijet Theoretical Uncertainties $e^{+}p$ }}{134}{figure.D.6}
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\addvspace {10\p@ }
\addvspace {10\p@ }
\addvspace {10\p@ }
\contentsline {figure}{\numberline {H.1}{\ignorespaces Polarized $e^-p$ and $e^+p$ $Q^2$ Inclusive-Jet Cross sections}}{159}{figure.H.1}
\contentsline {figure}{\numberline {H.2}{\ignorespaces Polarized $e^-p$ and $e^+p$ $\eta ^{\unhbox \voidb@x \hbox {\relax \fontsize {6}{7}\selectfont jet}}$ Inclusive-Jet Cross sections}}{160}{figure.H.2}
\contentsline {figure}{\numberline {H.3}{\ignorespaces Polarized $e^-p$ and $e^+p$ $x$ Inclusive-Jet Cross sections}}{160}{figure.H.3}
