Let me remind Almgren's regularity Theorem: the singular set of area-minimizing surface has codimension at least $2$. I wish to share here a simple example in low dimension, although I don't know whether the manifold is really a minimizer (this is the question).
The dimension of the manifold is two. Its co-dimension is $2$ as well. The ambient space ${\mathbb R}^4$ is identified with the space $M_2({\mathbb R})$ of $2\times2$ matrices. The Euclidian norm is $$\|A\|=\left(\frac12{\rm Tr}A^TA\right)^{1/2}.$$ It is normalized so that $\|I_2\|=1$.
The orthogonal group $O_2({\mathbb R})$ is a curve contained in the unit sphere $S_3$. It is made of two unit circles $\cal R$ and $\cal S$, respectively that of rotations and that of symmetries (I like to recall that, within the $3$-dimensional sphere, $\cal R$ and $\cal S$ are linked).
We look for a minimizing surface $\Gamma$ with boundary $O_2({\mathbb R})$. If it was unique, then it would inherit the symmetry of $O_2({\mathbb R})$. In particular, it should satisfy $$O_2({\mathbb R})\cdot\Gamma=\Gamma=\Gamma\cdot O_2({\mathbb R}).$$ This means that $\Gamma$ would be a union of orbits under the action of $O_2({\mathbb R})\times O_2({\mathbb R})$. Equivalently, $\Gamma$ would be defined in terms of singular values only. However, a single orbit, when the singular values are given and distinct ($s_1>s_2>0$), is already a surface, a $2$-dimensional object. Since the set of pairs $(s_1,s_2)$ must vary continuously from $(1,1)$, it seems therefore impossible that $s_1\ne s_2$. In conclusion, the only symmetric candidate is the surface $\Gamma_0$ defined by $s_1=s_2$. This is the union of the unit disks whose boundaries are $\cal R$ and $\cal S$.
The surface $\Gamma_0$ is singular at the origin $0_2$. The singularity is of codimension $2$, according to Almgren's Theorem. Its area is $2\pi$. My question is
Does $\Gamma_0$ minimize the area, among all the surfaces whose boundary is $O_2({\mathbb R})$ ?
Remark that the distance of any two points taken in $\cal R$ and $\cal S$ equals $\sqrt2$. One may consider the not-that-much symmetric surface $\Gamma_1$, the runion of segments $[R_\theta,S_\theta]$ where $$R_\theta=\begin{pmatrix} \cos\theta & \sin\theta \\ -\sin\theta & \cos\theta \end{pmatrix},\qquad S_\theta=\begin{pmatrix} \cos\theta & \sin\theta \\ \sin\theta & -\cos\theta \end{pmatrix}.$$ Notice that $\Gamma_1$ is not a critical point of the area functional. Actually it is contained in the unit sphere associated with the operator norm (definitely not a Euclidian one !) ; each point is therefore exposed. Its area, equal to $(\sqrt2+\log(1+\sqrt2)\pi$, exceeds that of $\Gamma_0$, because of $$\log(1+\sqrt2)=\int_1^{1+\sqrt2}\frac{ds}s>\frac{\sqrt2}{1+\sqrt2}=2-\sqrt2.$$