Let $\mathcal{L}(E)$ the algebra of all bounded linear operators on a complex Hilbert space $E$.
Let $B_n$ be the open unit ball of $\mathbb{C}^n$ and $\sigma$ be the normalized positive Borel measure on the unit sphere $\partial B_n$.
By this (book), we have $$\int_{\partial B_n} |\lambda_i|^2 d \sigma(\lambda)=\frac1n,$$ and $$\int_{\partial B_n} \lambda_i\overline{\lambda_j} d \sigma(\lambda)=0,\;\;\forall i,j\in\{1,...,n\}\;\text{with}\;i\neq j. $$
I don't understand this notation $\int_{\partial B_n} |\lambda_i|^2 d \sigma(\lambda)$ i.e. here is $\lambda=(\lambda_1,\cdots,\lambda_n)\in \partial B_n$?
Also
If $T_1,\cdots,T_n\in \mathcal{L}(E)$, why $$\sup_{(\lambda_1,\cdots,\lambda_n)\in \partial B_n}\langle (\sum_{i=1}^n \lambda_i T_i)h, (\sum_{i=1}^n \overline{\lambda_i} T_i^*)h \rangle\geq \int_{\partial B_n}\sum_{i,j=1}^n\lambda_i\overline{\lambda_j}\langle T_iT_j^* h, h\rangle d \sigma(\lambda)?$$