In the book of "Classical Fourier Analysis" by Loukas Grafakos, I am confused by the following detail, the author says that
$$\int_{\mathbb{S}^{n-1}}\theta^{\alpha}d\theta$$ is $0$ when at least one $\alpha_{j}$ is odd, why?
My attemption: suppose that $\alpha_{1}$ is odd then we can split the integral $\int_{\mathbb{S}^{n-1}}\theta^{\alpha}d\theta$ into two parts according the sign of $\theta_{1}$, we denote $\mathbb{S}^{n-1}_{+}$ the positive $\theta_{1}$ part and $\mathbb{S}^{n-1}_{-}$ the negtive $\theta_{1}$ part, and so we write $$\int_{\mathbb{S}^{n-1}}\theta^{\alpha}d\theta=\int_{\mathbb{S}_{+}^{n-1}}\theta^{\alpha}d\theta+\int_{\mathbb{S}_{-}^{n-1}}\theta^{\alpha}d\theta$$ We make the change of variable $\theta_{1}$ to $-\theta_{1}$ in the integral $$\int_{\mathbb{S}_{-}^{n-1}}\theta^{\alpha}d\theta$$ can we get $$\int_{\mathbb{S}_{-}^{n-1}}\theta^{\alpha}d\theta=-\int_{\mathbb{S}_{+}^{n-1}}\theta^{\alpha}d\theta$$?
Is sphere measure $d\theta$ invariant under the reflection $\theta_{1}\to-\theta_{1}$ transformation?
Notation: $\mathbb{S}^{n-1}$ is the sphere in $n$ dimension Euclidean space and $d\theta$ is surface measure on sphere, $\alpha=(\alpha_{1},\dots,\alpha_{n})\in\mathbb{Z}^{n}_{+}$,$\theta=(\theta_{1},\dots,\theta_{n})\in\mathbb{S}^{n-1}$, $\theta^{\alpha}=\theta_{1}^{\alpha_{1}}\theta_{2}^{\alpha_{2}}\cdots\theta_{n}^{\alpha_{n}}$
For any $n\in\mathbb{N}$, let $B_n(\mathbf{0}_n;1)=\{\mathbf{x}\in\mathbb{R}^n:|\mathbf{x}|_2\leq1\}$ and $S_{n-1}=\{\mathbf{u}\in\mathbb{R}^n:|\mathbf{u}|_2=1\}$.
where $|\mathbf{x}|^2_2=\sum^n_{k=1}x^2_k$ for all $\mathbf{x}=[x_1,\ldots,x_n]^\intercal\in\mathbb{R}^n$. Notice that $$B_n(\mathbf{0}_n;1)=\{(\mathbf{y},z)\in\mathbf{R}^{n-1}\times\mathbb{R}: |\mathbf{y}|_2\leq1,\, |z|\leq\sqrt{1-|\mathbf{y}|_2}\}$$
For $\alpha\in\mathbb{Z}^n_+$, consider the integral $$I_\alpha:=\int_{B_n(\mathbf{0}_n;1)}\mathbf{x}^\alpha\,dx_1\ldots dx_n$$ where $\mathbf{x}^\alpha=x^{\alpha_1}_1\cdot\ldots\cdot x^{\alpha_n}_n$ Using spherical coordinates $$I_{\alpha}=\int^1_0r^{n+|\alpha|_1-1}\int_{\mathbb{S}_{n-1}}\mathbf{u}^\alpha\,\sigma_{n-1}(d\mathbf{u})=\frac{1}{n+|\alpha|_1}\int_{\mathbb{S}_{n-1}}\mathbf{u}^\alpha\sigma_{n-1}(d\mathbf{u})$$ where $|\alpha|_1=\sum^n_{k=1}\alpha_k$, and $\sigma_{n-1}$ is the Lebesgue (surface) measure on the unit sphere $\mathbb{S}_{n-1}$. Notice that for any unitary transformation $U\in L(\mathbb{R}^n)$ where $U^\intercal U=UU^\intercal =I_n$), $U(B(\mathbf{0}_n;1)=B_n(\mathbf{0}_n;1)$ and $|\operatorname{det}(U)|=1$; hence $$I_{\alpha}=\int_{B_n(\mathbf{0}_n;1)}\mathbf{u}^\alpha\,d\mathbf{u}=\int_{B_n(\mathbf{0}_n;1)}(U\mathbf{u})^\alpha\,d\mathbf{u}$$ In particular, for any permutation $\tau(\alpha_1,\ldots,\alpha_n)=(\alpha_{\tau(1)},\ldots,\alpha_{\tau(n)})$ we have that $$I_{\alpha}=I_{\tau(\alpha)}$$ Consequently, if $\alpha_k\equiv1\mod 2$, we may assume without loss of generality that $k=n$. By Fubini's theorem $$I_{\alpha}=\int_{B_{n-1}(\mathbf{0}_{n-1};1)} y^{\alpha_1}_1\cdot\ldots\cdot y^{\alpha_{n-1}}_{n-1}\Big(\int^{\sqrt{1-|\mathbf{y}|_2}}_{-\sqrt{1-|\mathbf{y}|_2}} z^{\alpha_n}\,dz\Big)\,dy_1\ldots dy_{n-1}=0 $$ since $\int^a_{-a} z^{\alpha_n}\,dz=0$ for all $a>0$. This implies that $$\int_{\mathbf{S}_{n-1}}\mathbf{u}^\alpha\sigma_{n-1}(d\mathbf{u})=0$$ whenever $\sigma\in\mathbb{Z}^n_+$ has an odd component.