I'm taking a linear algebra course and the professor included the problem that prove $$ \rm{det}(I+\epsilon A) = 1 + \epsilon\,\rm{tr}\,A + o(\epsilon) $$ Since the professor hasn't covered the concept of eigenvalue, we are not recommended to mention eigenvalue in the solution. How to prove the equation by only using Laplace theorem?
Find the expansion for $\det(I+\epsilon A)$ where $\epsilon$ is small without using eigenvalue.
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Consider this expression of the determinant: $$ \det(B) = \sum_{\sigma \in S_n} (-1)^\sigma \prod_{i=1}^n b_{i,\sigma_i} $$
For $\sigma=id$, we have the term $b_{11}b_{22}\cdots b_{nn}$. Now take $B=I+\epsilon A$ and this term becomes $(1+\epsilon a_{11})(1+\epsilon a_{22})\cdots(1+\epsilon a_{nn})=1+\epsilon \, \rm{tr}\,A+$ higher-order terms.
All other terms in the expression above contain $\epsilon^{2}$.
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How this is done would depend on which characterizations of the determinant function you've seen. One of those is $$ \sum\left\{ \prod_{k=1}^n (\pm1)a_{k,\sigma(k)} : \sigma\text{ permutes }\{1,\ldots,n\} \right\} $$ where the sign is $+1$ if $\sigma$ is an even permutation and $-1$ if it is odd. When $\sigma$ is the identity permutation, the product is $$ (1+\varepsilon a_{11})\cdots(1+\varepsilon a_{nn}) = 1 + \varepsilon(a_{11}+\cdots+a_{nn}) + \varepsilon^2(\cdots) + \varepsilon^3(\cdots)+\cdots. $$ When $\sigma$ is any other permutation then the product is $$ \varepsilon a_{k,\sigma(k)} \varepsilon a_{j,\sigma(j)}\cdots+\cdots, $$ i.e. there are at least two indices $k$ for which $\sigma(k)\ne k$, so that $\varepsilon^2$ is a factor in this term. Thus the determinant is $$ 1+\varepsilon\operatorname{tr}(A)+(\text{terms of degree $\ge2$ in $\varepsilon$}). $$
We note that the determinant is defined by the Leibniz formula:
$$\det(\mathbf{I}+\epsilon\mathbf{A})=\sum_{\sigma \in S_{n}}\prod_{i=1}^{n}(\mathbf{I}+\epsilon \mathbf{A})_{i,\sigma_{i}} \cdot \operatorname{sgn}(\sigma)$$
We note that along the main diagonal we have:
$$\prod_{i=1}^{n}(\mathbf{I}+\epsilon \mathbf{A})_{i,i}=1+\epsilon (A_{11}+\cdots+A_{nn})+\mathcal{O}(\epsilon^{2})$$
And along the other possible permutations we have at best $\mathcal{O}(\epsilon^{2})$ as there must be at least 2 off-diagonal entries for it to be a vaid permutation. Therefore we can say:
$$\det(\mathbf{I}+\epsilon\mathbf{A})=1+\epsilon\operatorname{Tr}(\mathbf{A})+\mathcal{O}(\epsilon^{2})$$
As required.