Step 1: Path independence and conservative field.
If the line integral of a vector field \(\vec{F} = (F_1, F_2, F_3)\) is path-independent, the field is conservative. This implies there exists a scalar potential function \(f(x, y, z)\) such that:
\[
F_1 = \frac{\partial f}{\partial x}, \quad F_2 = \frac{\partial f}{\partial y}, \quad F_3 = \frac{\partial f}{\partial z}.
\]
Step 2: Line integral over a closed path.
For conservative fields, the line integral over any closed path is zero. Mathematically, this is expressed as:
\[
\oint_\Gamma \vec{F} \cdot d\vec{r} = 0.
\]
Step 3: Curl condition for a conservative field.
A necessary condition for a field to be conservative is that its curl must vanish:
\[
{curl } \vec{F} = \nabla \times \vec{F} = 0.
\]
This leads to the component-wise conditions:
\[
\frac{\partial F_2}{\partial x} = \frac{\partial F_1}{\partial y}, \quad \frac{\partial F_3}{\partial y} = \frac{\partial F_2}{\partial z}, \quad \frac{\partial F_1}{\partial z} = \frac{\partial F_3}{\partial x}.
\]
Final Answer:
\[
\boxed{{(1, 2, 4)}}
\]