I think there is a possible reduction of this questionis true (homotopy implies isotopy). Consider a generic smooth torus embedding $f: T^2 \to S^1\times S^4$, then the projection to $S^1$ gives a circle-valued Morse function on $T^2$. Because of the ambient dimension (codimension 3), I think one may isotope $f$ to cancel critical points and obtain an isotopic embedding $f': T^2\to S^1\times S^4$ such that the projection to $S^1$ has no critical points when restricted to $T^2$ if the map $f_{|T^2}:T^2\to S^1$ is homotopically non-trivial. Thus $f'^{-1}(z)$ is a union of $k$ circles in $S^4$ for all $z\in S^1$, where $k$ is the index of $\pi_1(T^2)\to \pi_1(S^1)$. The homotopy type of $f'$ should be determined by the number of circles, or correspondingly the index of the image $\pi_1(T^2)\to \pi_1(S^1)$.$k$
IfFor the configuration spacehomotopically trivial case, I think the technique of the $k$ circlesWhitney-Wu unknotting theorem implies that any two homotopically trivial tori embedded in $S^4$ has $\pi_1$ isomorphic$S^1\times S^4$ are isotopic. The point is that we may use Morse theory to shrink the symmetric grouptorus down into an $S_k$$I\times S^4$ slice, then I think that one should be able to show that any two such maps are isotopicapply Whitney-Wu.
For $k=1$, ieNow consider the homotopically non-trivial case that, where $f'^{-1}(z)$ has$f’^{-1}(z)$ consists of $k$ circles for every $z$. We may think of this as a single circlemap $g: S^1 \to Emb(\sqcup^k S^1, S^4)$, I think one can showwhere the monodromy permutes the components of $\sqcup^k S^1$ cyclically so that all such tori are isotopicthe mapping torus is a torus. Because thisThen $g(1)$ is codimensionan embedding of $3$ in$\sqcup^k S^1$ to $S^4$ it is unknotted.
Let $f: S^1 \times S^1 \to S^4$ be$g(1)=\gamma_1 \sqcup \cdots \sqcup \gamma_k$ a map sodisjoint union of circles. By general position, this is the boundary of an embedding $D^2_1 \sqcup \cdots \sqcup D^2_k$. Assume that the monodromy sends $f(z,S^1)$ is embedded for all$\gamma_i$ to $z$$\gamma_{i+1}$, then weindices taken $(\mod k)$. We may think ofextend $f$ as a loop in in the configuration space of embeddings$g$ to an ambient isotopy of a circle in $S^4$, and hence get a path $G: [0,1] \to Emb( \sqcup^k D^2 , S^4)$ with boundary restricting to $g$. This loop We may be achieved by a 1-parameter family of diffeomorphismsalso assume that $D_i$ is taken to $D_{i+1}$ by ambientthe isotopy. Let $D$ be an embedded disk bounding, $\gamma= f(1,S^1)$$1\leq i< k$, and let $D'$ be the disk obtained after the ambient isotopy$D_k$ is taken to $D_1’$ with $\partial D_1’=\gamma_1$.
By the 4-dimensional light-bulb theorem (Theorem 1.10), $D$$D_1$ is isotopic to $D'$$D_1'$ rel $\gamma$$\gamma_1$. So By general position, we may assume that this isotopy misses $D_2, \ldots, D_k$ (since these all sit inside of disjoint balls).
So this isotopy may be achieved by a 1-parameter isotopy of disks $G’:S^1 \to Emb(\sqcup^k D^2,S^4)$. But any such isotopy is homotopic to the constant isotopya cyclic rotation of order $k$. Consider a point on the disk $D_1$, the point gives a loop in $S^4$ by iterating the isotopy $k$ times, which is contractible, and hence one may assume that the isotopy fixes this point the points on the disks $D_1, \dots, D_k$ arranged around a round circle. Then one may also assume that the tangent space to the diskdisks at the point is fixedare permuted cyclically, and then that the disks are fixedpermuted by a rotation by shrinking them down to the tangent space. Hence I think that the tori with $\pi_1(T^2)\to \pi_1(S^1\times S^4)$ surjectivethere should be isotopic to the product torusonly one isotopy class of embedded tori for each $k$.
ForIt’s possible that the homotopically trivial caseapplication of the 4D lightbulb trick here is overkill, one might be able to use the technique oflook at the Whitney-Wu unknotting theoremclassical isotopy theory linked to prove that any two homotopically trivial tori are isotopic; certainly their liftsabove to the universal coversee if it can be applied directly to show that homotopy implies isotopy in this case (or a large enough finite-sheeted cover) willthings tend to be isotopicmore flexible in higher dimensions).