  Fluctuation-induced forces are investigated for ideal and imperfect Bose
gases confined to $d$-dimensional films of size $\infty^{d-1}\times D$ under
periodic (P), antiperiodic (A), Dirichlet-Dirichlet (DD), Neumann-Neumann (NN),
and Robin (R) boundary conditions (BCs). The full scaling functions
$\Upsilon^{\text{BC}}_d(x_\lambda=D/\lambda_{th},{x_\xi=D/\xi})$ of the
residual reduced grand potential per area,
$\varphi_{\text{res},d}^{\text{BC}}(T,\mu,D)=D^{-(d-1)}\Upsilon_d^{\text{BC}}(x_\lambda,x_\xi)$,
are determined for the ideal gas case with these BCs, where $\lambda_{th}$ and
$\xi$ are the thermal de-Broglie wavelength and the bulk correlation length,
respectively. The scaling functions $\Theta^{\text{BC}}_d(x_\xi)\equiv
\Upsilon_d^{\text{BC}}(\infty,x_\xi)$ describing the critical behavior at the
bulk condensation transition are shown to agree with those previously
determined from a massive free $O(2)$ theory for
$\text{BC}=\text{P},\text{A},\text{DD},\text{DN},\text{NN}$. For $d=3$, they
are expressed in closed analytical form. The analogous functions
$\Upsilon_d^{\text{BC}}(x_\lambda,x_\xi,c_1D,c_2D)$ and
$\Theta^{\text{R}}_d(x_\xi,c_1D,c_2D)$ under the RBCs
$(\partial_z-c_1)\phi|_{z=0}=(\partial_z+c_2)\phi|_{z=D}=0$ with $c_1\ge 0$ and
$c_2\ge 0$ are also determined. The functions
$\Upsilon_{\infty,d}^{\text{P}}(x_\lambda,x_\xi)$ and
$\Phi_{\infty,d}^{\text{P}}(x_\xi)$ for the imperfect Bose gas are shown to
agree with those of the interacting Bose gas with $n\to\infty$ internal degrees
of freedom. Hence for ${d=3}$, $\Phi_{\infty,d}^{\text{P}}(x_\xi)$ is known
exactly in closed analytic form. A modified imperfect Bose-gas model with free
BC is introduced that corresponds to the limit $n\to\infty$ of this interacting
Bose gas. Exact results for the function
$\Theta_{\infty,3}^{\mathbb{DD}}(x_\xi)$ therefore follow from those of the
$O(2n)$ $\phi^4$ model for $n\to\infty$.
