The Special Lagrangian Potential Equation for a function $u$ on a domain $Omegasubset {bf R}^n$ is given by ${rm tr}{arctan(D^2 ,u) } = theta$ for a contant $theta in (-n {piover 2}, n {piover 2})$. For $C^2$ solutions the graph of $Du$ in $Omegatimes {bf R}^n$ is a special Lagrangian submanfold. Much has been understood about the Dirichlet problem for this equation, but the existence result relies on explicitly computing the associated boundary conditions (or, otherwise said, computing the pseudo-convexity for the associated potential theory). This is done in this paper, and the answer is interesting. The result carries over to many related equations -- for example, those obtained by taking $sum_k arctan, lambda_k^{{mathfrak g}} = theta$ where ${{mathfrak g}} : {rm Sym}^2({bf R}^n)to {bf R}$ is a Garding-Dirichlet polynomial which is hyperbolic with respect to the identity. A particular example of this is the deformed Hermitian-Yang-Mills equation which appears in mirror symmetry. Another example is $sum_j arctan kappa_j = theta$ where $kappa_1, ... , kappa_n$ are the principal curvatures of the graph of $u$ in $Omegatimes {bf R}$. We also discuss the inhomogeneous Dirichlet Problem ${rm tr}{arctan(D^2_x ,u)} = psi(x)$ where $psi : overline{Omega}to (-n {piover 2}, n {piover 2})$. This equation has the feature that the pull-back of $psi$ to the Lagrangian submanifold $Lequiv {rm graph}(Du)$ is the phase function $theta$ of the tangent spaces of $L$. On $L$ it satisfies the equation $ abla psi = -JH$ where $H$ is the mean curvature vector field of $L$.
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