Suppose that $A_{2\times 2}$ is a hermitian matrix, so it has real eigenvalues $\lambda_1$ and $\lambda_2$ and corresponding orthonormal eigenvectors $\underline u_1$ and $\underline u_2$ and we know it can be written as the sum of two $rank-1$ hermitian matrices: $\text{T is the symbol for transpose and * for complex conjugate}$
$$A=\lambda_1\underline u_1\otimes\underline u_1+\lambda_2\underline u_2\otimes\underline u_2=\lambda_1\underline u_1\underline u_1^{*T}+\lambda_2\underline u_2\underline u_2^{*T}\qquad $$
Both $\underline u_1\otimes \underline u_1$ and $\underline u_2\otimes \underline u_2$ are hermitian so $(\underline u_1\otimes \underline u_1+ \underline u_2\otimes \underline u_2)$ is hermitian. In a book on page 50, it says that:
As the two unit orthogonal eigenvectors verify $\underline u_1\underline u_1^{*T}+\underline u_2 \underline u_2^{*T}=I_{D2}$, it follows the Chandrasekhar decomposition of the wave given by $$J=(\lambda_1-\lambda_2)\underline u_1\underline u_1^{*T}+\lambda_2I_{D2}=J_{CP}+J_{CD}$$
My question is what do we mean by $I_{D2}$ matrix?
Also what is Chandrasekhar decomposition? Can you introduce me online resources to study?
Or can you guide me to the Chanrasekhar's original paper in which he introduced this decomposition?