The work done by a moving particle is given by the formula:
\[
W = \int_{\mathbf{r_1}}^{\mathbf{r_2}} \mathbf{F} \cdot d\mathbf{r}
\]
where:
- \( \mathbf{F} = 6x^2 \hat{i} + (3xz + y) \hat{j} + 4z \hat{k} \) is the force field,
- \( \mathbf{r_1} = (0,0,0) \) and \( \mathbf{r_2} = (1,2,3) \) are the initial and final positions,
- \( d\mathbf{r} = dx \hat{i} + dy \hat{j} + dz \hat{k} \) is the infinitesimal displacement vector.
The work integral will be evaluated along the straight line from (0,0,0) to (1,2,3). To parameterize the path, we write:
\[
x = t, \quad y = 2t, \quad z = 3t \quad \text{where} \quad t \in [0,1].
\]
The differentials are:
\[
dx = dt, \quad dy = 2dt, \quad dz = 3dt.
\]
Substitute into the force equation:
\[
\mathbf{F} = 6x^2 \hat{i} + (3xz + y) \hat{j} + 4z \hat{k}.
\]
Now, calculate the dot product \( \mathbf{F} \cdot d\mathbf{r} \):
\[
\mathbf{F} \cdot d\mathbf{r} = (6x^2 \, dx) + (3xz + y) \, dy + (4z \, dz).
\]
Substitute the expressions for \( x \), \( y \), and \( z \) into the equation. After integrating over the given bounds from 0 to 1, we find that:
\[
W = 28.
\]
Thus, the work done by the particle is \( \boxed{28} \) (in integer).