I am trying to read Exploring the toolkit of Jean Bourgain, a beautiful article by Terrence Tao, that can be found here. At page 5 Tao considers the integral
$$ \int_{|\xi|\le \delta/ t_j}| \hat{1}_B(\xi) |^2 \hat{\sigma}(t_j\xi) d \xi \tag{1} $$
where $0< \delta= \delta(\epsilon) \le 1/2$ is a small quantity depending on $0<\epsilon< 1/2$ to be chosen later, $B \subset [-1,1]^2$, $0<t_j \le 1$, $\hat{1}_B$ is the Fourier transform of the indicator function $1_B$, i.e.,
$$ \hat{1}_B(\xi) = \int_{\mathbb{R}^d} 1_B(x) e^{2\pi i x \xi} dx , $$
and $\hat{\sigma}(\xi) = \int_{S^1} e^{-2\pi i \omega \xi} d \sigma( \omega) $ is the Fourier transform of the surface measure $d \sigma$ on the unit circle $S^1$.
Tao states that, for $\delta$ small enough the factor $\hat{\sigma}(t_j\xi)$ is close to $1$ and thus it is not difficult to show that the integral in $(1)$ is approximately $\gtrsim|B|$, thus
$$ \int_{|\xi|\le \delta/ t_j}| \hat{1}_B(\xi) |^2 \hat{\sigma}(t_j\xi) d \xi \gtrsim |B| \ge \epsilon^2 . $$
How does one rigorously show this?