[step:Recall the Besov norm and Bernstein's inequality]
Fix a Littlewood–Paley resolution of unity as in the previous proofs: $\varphi_0, \varphi \in C^\infty_c(\mathbb{R}^n)$ with $\varphi_0$ supported in $\{|\xi|\le 2\}$, $\varphi$ supported in $\{1/2\le|\xi|\le 2\}$, $\varphi_0 + \sum_{j\ge 1}\varphi(2^{-j}\cdot) = 1$. Set $\varphi_j(\xi) := \varphi(2^{-j}\xi)$ and define the Littlewood–Paley projectors
\begin{align*}
\Delta_j : \mathcal{S}'(\mathbb{R}^n) &\to \mathcal{S}'(\mathbb{R}^n) \\
f &\mapsto \mathcal{F}^{-1}(\varphi_j\,\hat f\,), \qquad j \ge 0.
\end{align*}
The Besov norm for parameters $(s, p, q)$ is
\begin{align*}
\|f\|_{B^s_{p,q}(\mathbb{R}^n)} := \Bigl(\sum_{j=0}^\infty 2^{jsq}\,\|\Delta_j f\|_{L^p(\mathbb{R}^n)}^q\Bigr)^{1/q}, \qquad 1 \le q < \infty,
\end{align*}
with the obvious modification $\sup_{j\ge 0} 2^{js}\,\|\Delta_j f\|_{L^p}$ for $q = \infty$.
Recall the [Bernstein Inequality for Littlewood–Paley Pieces](/theorems/???) in its $L^p$-to-$L^{p_1}$ form: if $g \in \mathcal{S}'(\mathbb{R}^n)$ has $\hat g$ supported in the ball $\{|\xi| \le R\}$ and $g \in L^{p_0}$ for some $1 \le p_0 \le \infty$, then for any $p_1$ with $p_0 \le p_1 \le \infty$,
\begin{align*}
\|g\|_{L^{p_1}(\mathbb{R}^n)} \le C_{n,p_0,p_1}\,R^{n(1/p_0 - 1/p_1)}\,\|g\|_{L^{p_0}(\mathbb{R}^n)}.
\end{align*}
Apply this to $\Delta_j f$ for each $j \ge 0$. The function $\Delta_j f$ has Fourier support in $\{|\xi|\le 2^{j+1}\}$ (in the ball of radius $2^{j+1}$), so $R = 2^{j+1}$. Hence
\begin{align*}
\|\Delta_j f\|_{L^{p_1}} \le C_{n,p_0,p_1}\,2^{(j+1)n(1/p_0 - 1/p_1)}\,\|\Delta_j f\|_{L^{p_0}} \le C'_{n,p_0,p_1}\,2^{jn(1/p_0 - 1/p_1)}\,\|\Delta_j f\|_{L^{p_0}}
\end{align*}
where $C'_{n,p_0,p_1} := 2^{n(1/p_0-1/p_1)}\,C_{n,p_0,p_1}$ absorbs the constant factor $2^{n(1/p_0 - 1/p_1)}$ from the $j+1$ shift.
[/step]