TFPT scientific source excerpt Original repository path: documents/archive--tfpt-45--source_extracts--01_boundary_kernel_source/sections/001-section-primitive-core-and-carrier-interface-handoff.tex Original file SHA-256: 7d6e673d99c29d950dc601283cd51c1cc0b113567eeb79c8396fec9c82a02c79 Inclusive original lines: 65-155 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000065 | \begin{definition}[One-sided boundary admissibility datum] 000066 | \label{def:reduced-theorem-datum} 000067 | The one-sided boundary admissibility datum is 000068 | \[ 000069 | \Tbound:=(\mathcal A_+,\mathcal H_+,D_+,J,\Gamma,B_\Sigma) 000070 | \] 000071 | with the following built-in admissibility conditions: 000072 | \begin{enumerate}[label=(\roman*), leftmargin=1.5em, topsep=3pt, itemsep=2pt] 000073 | \item $Z(\mathcal A_+)$ is spectrally regular and its Gelfand spectrum is a smooth compact oriented manifold with boundary $M_+$; 000074 | \item $B_\Sigma$ is a self-adjoint tangential boundary operator on $\Sigma:=\partial M_+$ compatible with the boundary restrictions of $J$ and $\Gamma$; 000075 | \item in a collar neighborhood of $\Sigma$, the Dirac operator has canonical product form 000076 | \[ 000077 | D_+=\gamma_n(\partial_n+B_\Sigma); 000078 | \] 000079 | \item the boundary collar is reflection-regular so that canonical doubling, the Calder\'on projector, and the admissibility complex are well posed on the same datum. 000080 | \end{enumerate} 000081 | \end{definition} 000082 | 000083 | \begin{remark}[Almost-commutative realizations] 000084 | \label{ass:almost-commutative-factorization} 000085 | When a factorized realization is useful, one may choose 000086 | \[ 000087 | \mathcal H\cong L^2(\widetilde M,S)\otimes \Hint, 000088 | \] 000089 | with $S\to\widetilde M$ the spinor bundle on the oriented double cover and $\Hint$ a finite 000090 | internal Hilbert space. This is an analytic realization choice rather than part of the boundary 000091 | datum. 000092 | \end{remark} 000093 | 000094 | \begin{theorem}[Doubling, deck involution, and boundary polarization] 000095 | \label{thm:primitive-datum-from-reduced-datum} 000096 | \label{thm:primitive-scaffold-from-reduced-datum} 000097 | Let $\Tbound$ be as above. Let 000098 | \[ 000099 | \widetilde M:=M_+\cup_{\Sigma} M_+^{\mathrm{op}} 000100 | \] 000101 | be the doubled manifold and let 000102 | \[ 000103 | \taudbl:\widetilde M\to\widetilde M 000104 | \] 000105 | be its deck involution. Let $P_C$ be the Calder\'on projector of the APS-realized boundary problem 000106 | for $D_+$ on $\Sigma$, and define the boundary polarization operator 000107 | \[ 000108 | \iC:=2P_C-1 000109 | \] 000110 | on the Cauchy-data Hilbert space $\mathcal H_{\partial}$. 000111 | 000112 | Then: 000113 | \begin{enumerate}[label=(\roman*), leftmargin=1.8em, topsep=3pt, itemsep=2pt] 000114 | \item the geometric objects are 000115 | \[ 000116 | M=\widetilde M/\taudbl, 000117 | \qquad 000118 | \Seam=\mathrm{Fix}(\taudbl), 000119 | \qquad 000120 | \Xbulk=\widetilde M\setminus\Seam; 000121 | \] 000122 | \item the doubled operator and its even and odd parts are 000123 | \[ 000124 | D=D_+\cup_{\Sigma}D_+^{\mathrm{op}}, 000125 | \qquad 000126 | D_{\mathrm{ref}}:=\frac12\bigl(D+\taudbl^{\ast}D\taudbl^{\ast}\bigr), 000127 | \qquad 000128 | D_{\mathrm{rel}}:=\frac12\bigl(D-\taudbl^{\ast}D\taudbl^{\ast}\bigr); 000129 | \] 000130 | \item on boundary Cauchy data the induced reflection $R_{\taudbl}$ satisfies 000131 | \[ 000132 | \operatorname{Ran}(P_C)=\ker(R_{\taudbl}-1), 000133 | \qquad 000134 | \ker(P_C)=\ker(R_{\taudbl}+1), 000135 | \qquad 000136 | \iC=R_{\taudbl}. 000137 | \] 000138 | \end{enumerate} 000139 | Hence the primitive scaffold 000140 | \[ 000141 | \Tprim^{\mathrm{kin}} 000142 | := 000143 | (\Xbulk,\widetilde M,M,\Seam,\taudbl,\iC,D_{\mathrm{ref}},D_{\mathrm{rel}},\chiseed) 000144 | \] 000145 | is derived, not assumed. The derived doubled datum may be recorded as 000146 | \[ 000147 | \Tmin^{\mathrm{cl}}:=(\mathcal A,\mathcal H,D,J,\Gamma,\taudbl,\iC), 000148 | \] 000149 | If one further chooses an almost-commutative factorization 000150 | \[ 000151 | \mathcal H_{\mathrm{prim}}\cong L^2(\Xbulk,S)\otimes \Hint, 000152 | \] 000153 | then $S$ and $\Hint$ refer only to that chosen realization and are not additional 000154 | reconstruction outputs. 000155 | \end{theorem}