Step 1: A useful way to see this without directly writing the characteristic polynomial is to think in terms of the Jordan canonical form of $A$ (over $\mathbb{C}$, which every real matrix also possesses after extending scalars).
Step 2: Every $n \times n$ matrix $A$ has a Jordan form made of Jordan blocks whose sizes add up to exactly $n$. If a matrix has a single eigenvalue $c$, the simplest case is one Jordan block of size $n$ for $c$, attained for instance when $A$ is diagonalizable with every eigenvalue equal to $c$, i.e. $A = cI_n$, which gives that eigenvalue an algebraic multiplicity of exactly $n$, using up the entire dimension of the matrix.
Step 3: Because the sum of all block sizes across all eigenvalues must equal $n$ exactly, this is just the dimension of the space the matrix acts on, a single eigenvalue can never claim more than $n$ of these dimensions, so $n$ is a hard ceiling on multiplicity.
Step 4: Since $A = cI_n$ is a genuine real matrix that reaches this ceiling, with $c$ appearing $n$ times, the ceiling of $n$ is not just a bound, it is actually reached. So the maximum multiplicity possible is $n$, ruling out $n-1$ (too small, since $n$ is achievable), $1$ (the multiplicity in the opposite extreme case of all-distinct eigenvalues, not the maximum), and $n+1$ (exceeds the degree of the characteristic polynomial and can never occur).
\[ \boxed{n} \]For the matrix, $A = \begin{bmatrix} -4 & 0 \\ -1.6 & 4 \end{bmatrix}$, the eigenvalues ($\lambda$) and eigenvectors ($X$) respectively are:
Consider the following matrix: \[ \begin{pmatrix} 0 & 1 & 1 & 1 \\ 1 & 0 & 1 & 1 \\ 1 & 1 & 0 & 1 \\ 1 & 1 & 1 & 0 \end{pmatrix} \] The largest eigenvalue of the above matrix is \(\underline{\hspace{2cm}}\).