\begin{document}$G_C$\end{document}, magnetic \begin{document}$G_M$\end{document}, and quadrupole \begin{document}$G_Q$\end{document} form factors with lattice data. The dressed form factors, \begin{document}$G_C^D$\end{document} and \begin{document}$G_M^D$\end{document}, exhibit good agreement with lattice results; however, \begin{document}$G_Q^D$\end{document} is found to be harder than what is observed in lattice calculations. The Rosenbluth cross section for elastic electron scattering on a spin-one particle can be expressed through the structure functions \begin{document}$A(Q^2)$\end{document} and \begin{document}$B(Q^2)$\end{document}. Additionally, the tensor polarization \begin{document}$T_{20}(Q^2,\theta)$\end{document} can also be formulated in terms of these form factors. We analyze the structure functions \begin{document}$A(Q^2)$\end{document}, \begin{document}$B(Q^2)$\end{document} and tensor polarization function \begin{document}$T_{20}(Q^2,\theta)$\end{document}; our findings quantitatively align with predicted values across various limits. In impact parameter space, we examine parton distribution functions along with their dependence on longitudinal momentum fraction x and impact parameter \begin{document}$\boldsymbol{b}_{\perp}$\end{document}. The width distributions in impact parameter space reveal that the range of the charge distribution \begin{document}$ q_C(x,\boldsymbol{b}_{\perp}^2)$\end{document} is the most extensive. In contrast, the transverse magnetic radius falls within a moderate range, while the quadrupole distribution \begin{document}$q_Q(x,\boldsymbol{b}_{\perp}^2) $\end{document} demonstrates the narrowest extent."> <i>ρ</i> meson form factors and parton distribution functions in impact parameter space -
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