Complete Lagrangian subspace characterization of self-adjoint boundary conditions

Let EqE_q be the fiber of the Hermitian vector bundle over a boundary point qq, let AnA^n be the self-adjoint normal principal-symbol operator on EqE_q, and let SqEqS_q\subseteq E_q be a subbundle. A subspace SEqS\subseteq E_q is complete Lagrangian relative to AnA^n when

S=S#,S=S^\#,

where

S#={ϕEq:(ϕAnχ)=0 χS}.S^\#=\{\phi\in E_q:(\phi\mid A^n\chi)=0\ \forall\chi\in S\}.

Complete Lagrangian boundary-condition conjecture. The boundary condition

ψ(q)SqqQ\psi(q)\in S_q\quad\forall q\in\partial\mathcal{Q}

can occur in a self-adjoint extension of HH from Cc(EQ)C_c^\infty(E|_{\mathcal{Q}^\circ}) in L2(E)L^2(E) if and only if SqS_q is a complete Lagrangian subspace of EqE_q relative to AnA^n for every qQq\in\partial\mathcal{Q}. This characterizes the reflecting boundary conditions compatible with self-adjointness; the paper presents it as the right condition for such boundary conditions.

Sources & referencesView supporting material

Primary source

Julian Schmidt, Stefan Teufel and Roderich Tumulka, “Interior-Boundary Conditions for Many-Body Dirac Operators and Codimension-1 Boundaries”, arXiv:1811.02947 (2019).

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