Concept:
Let \( A \) be an \( n \times n \) square matrix. If \( \lambda \) is an eigenvalue of \( A \) corresponding to a non-zero eigenvector \( X \), then by definition:
\[
AX = \lambda X
\]
Using matrix algebra and spectral properties, we can determine the eigenvalues of functions of matrices:
• Eigenvalues of an inverse matrix (\( A^{-1} \)): If \( A \) is non-singular, multiplying both sides of \( AX = \lambda X \) by \( A^{-1} \) gives \( X = \lambda A^{-1} X \), which transforms directly to \( A^{-1}X = \frac{1}{\lambda} X \). Thus, the eigenvalues are \( \frac{1}{\lambda} \).
• Eigenvalues of a scalar multiple matrix (\( kI \)): Since \( IX = X \), we have \( (kI)X = kX \). The eigenvalue of the identity matrix scaled by \( k \) is identically \( k \).
• Eigenvalues of matrix polynomials/combinations: If \( P(A) = c_m A^m + \cdots + c_1 A + c_0 I \), then the eigenvalues of \( P(A) \) are given exactly by \( P(\lambda) = c_m \lambda^m + \cdots + c_1 \lambda + c_0 \).
Step 1: Application of spectral mapping theorem to each component.
We are asked to find the eigenvalues of the linear matrix combination expression:
\[
B = A^{-1} + 2I + A
\]
Let \( X_i \) be the non-zero eigenvector associated with the specific eigenvalue \( \lambda_i \) of the square matrix \( A \). This means:
\[
AX_i = \lambda_i X_i \quad \text{for } i = 1, 2, 3.
\]
Step 2: Operating the matrix equation onto the eigenvector \( X_i \).
Let us apply the matrix combination expression \( B \) directly onto the eigenvector \( X_i \):
\[
BX_i = (A^{-1} + 2I + A)X_i
\]
Distributing the eigenvector vector multiplication over the matrix addition linearly:
\[
BX_i = A^{-1}X_i + 2IX_i + AX_i
\]
Step 3: Substituting known eigenvalue relations.
We substitute the fundamental eigenvalue properties for each standalone term inside the equation:
• For the matrix vector product \( A^{-1}X_i \), since \( A \) has eigenvalue \( \lambda_i \), its inverse operation satisfies \( A^{-1}X_i = \frac{1}{\lambda_i}X_i \).
• For the identity component product, \( 2IX_i = 2X_i \).
• For the primary matrix product, \( AX_i = \lambda_i X_i \).
Substituting these direct scalar equations back into our operational matrix-vector expansion:
\[
BX_i = \left(\frac{1}{\lambda_i}\right)X_i + 2X_i + \lambda_i X_i
\]
Step 4: Factoring out the common vector component to finalize the eigenvalue format.
We now safely factor out the common non-zero eigenvector \( X_i \) from the right side of the expression:
\[
BX_i = \left( \frac{1}{\lambda_i} + 2 + \lambda_i \right) X_i
\]
This precisely fits the standard eigenvalue-eigenvector functional definition \( BX_i = \mu_i X_i \), showing that the scalar multiplier value is the new eigenvalue.
Repeating this exact linear mapping process independently for all three eigenvalues \( \lambda_1, \lambda_2, \lambda_3 \), the complete set of new eigenvalues for the matrix \( A^{-1} + 2I + A \) is uniquely evaluated as:
\[
\frac{1}{\lambda_1} + 2 + \lambda_1, \quad \frac{1}{\lambda_2} + 2 + \lambda_2, \quad \text{and} \quad \frac{1}{\lambda_3} + 2 + \lambda_3
\]
This maps explicitly and without any sign alterations to Option (D).