From 4080ac0d71d9b83178a65be8edad8c746c96dcdb Mon Sep 17 00:00:00 2001 From: ShqWW Date: Mon, 28 Oct 2024 19:08:51 +0800 Subject: [PATCH] update --- main.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/main.tex b/main.tex index 7cde919..7923abb 100644 --- a/main.tex +++ b/main.tex @@ -188,7 +188,7 @@ However, the representation of lane anchors as rays presents certain limitations \begin{figure}[t] \centering \includegraphics[width=0.87\linewidth]{thesis_figure/coord/localpolar.png} - \caption{The local polar coordinate system. The ground truth of the radius $\hat{r}_{i}^{l}$ of the $i$-th local pole is defines as the minimum distance from the pole to the lane curve instance. A positive pole has a radius $\hat{r}_{i}^{l}$ that is below a threshold $\tau^{l}$, and vice versa. Additionally, the ground truth angle $\hat{\theta}_i$ is determined by the angle formed between the radius vector (connecting the pole to the closest point on the lanes) and the polar axis.} + \caption{The local polar coordinate system. The ground truth of the radius $\hat{r}_{i}^{l}$ of the $i$-th local pole is defines as the minimum distance from the pole to the lane curve instance. A positive pole has a radius $\hat{r}_{i}^{l}$ that is below a threshold $\lambda^{l}$, and vice versa. Additionally, the ground truth angle $\hat{\theta}_i$ is determined by the angle formed between the radius vector (connecting the pole to the closest point on the lanes) and the polar axis.} \label{lpmlabel} \end{figure} \par