\documentclass[english]{article} \usepackage[T1]{fontenc} \usepackage[latin9]{inputenc} \usepackage{units} \makeatletter \makeatother \usepackage{babel} \begin{document} \title{Nuclear modification of charged hadrons and jets in isobar collisions at $\sqrt{s_{\mathrm{NN}}}=\unit[200]{GeV}$ at STAR} \author{Isaac Mooney for the STAR Collaboration} \date{\today} \maketitle \begin{abstract} \thispagestyle{empty}Partonic scatterings with high momentum transfer occur before the formation of the quark-gluon plasma (QGP) in heavy-ion (A+A) collisions and result in collimated collections of hadrons called jets. The modification of the parton shower in the QGP compared to that in proton-proton (p+p) collisions offers insight into the nature of the medium's interaction with colored probes. Typically, this is measured as a ratio of hadron or jet spectra in A+A and p+p collisions called the $R_{\mathrm{AA}}$. The nominal RHIC A+A collision species is gold (Au) with 197 nucleons, but the high-statistics 2018 STAR isobar data from Zr+Zr and Ru+Ru collisions, each with 96 nucleons, offer the opportunity to study the system size dependence of nuclear modification of hard probes. \par In this talk, we present a measurement of the inclusive charged hadron $R_{\mathrm{AA}}$ differentially with average number of participants ($\left\langle N_{\mathrm{part}}\right\rangle $) in isobar collisions at STAR. The large available range of $\left\langle N_{\mathrm{part}}\right\rangle $ in these data allows for comparisons to small systems and Au+Au results. We also present ongoing work to control the path length of the partons through the medium via event shape engineering. Events are categorized by their eccentricity, and within a given eccentricity and centrality class, jets traveling in the event plane direction are compared to those traveling perpendicular to it, in order to study the dependence of jet energy loss on the collision geometry. \end{abstract} \end{document}