TFPT scientific source excerpt Original repository path: documents/archive--paper-latex--tfpt-42/sections/003-subsection-primitive-relative-spectral-dynamics.tex Original file SHA-256: 8683d7459140a06d5e03a06adefd05bf7e6538356e4e4da4397133aa991b8fe4 Inclusive original lines: 1-35 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. 000001 | \subsection{Primitive relative spectral dynamics} 000002 | 000003 | The carrier theorem is not intended to float above an unspecified microscopic dynamics. The 000004 | starting point is therefore the one-sided boundary datum from which the primitive layer, the 000005 | derived closed datum, and the canonical admissibility projector are reconstructed before the later 000006 | closure theorems are invoked. 000007 | 000008 | \begin{definition}[One-sided boundary admissibility datum] 000009 | \label{def:reduced-theorem-datum} 000010 | The one-sided boundary admissibility datum is 000011 | \[ 000012 | \Tbound:=(\mathcal A_+,\mathcal H_+,D_+,J,\Gamma,B_\Sigma) 000013 | \] 000014 | with the following built-in admissibility conditions: 000015 | \begin{enumerate}[label=(\roman*), leftmargin=1.5em, topsep=3pt, itemsep=2pt] 000016 | \item $Z(\mathcal A_+)$ is spectrally regular and its Gelfand spectrum is a smooth compact oriented manifold with boundary $M_+$; 000017 | \item $B_\Sigma$ is a self-adjoint tangential boundary operator on $\Sigma:=\partial M_+$ compatible with the boundary restrictions of $J$ and $\Gamma$; 000018 | \item in a collar neighborhood of $\Sigma$, the Dirac operator has canonical product form 000019 | \[ 000020 | D_+=\gamma_n(\partial_n+B_\Sigma); 000021 | \] 000022 | \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. 000023 | \end{enumerate} 000024 | \end{definition} 000025 | 000026 | \begin{remark}[Almost-commutative realizations] 000027 | \label{ass:almost-commutative-factorization} 000028 | When a factorized realization is useful, one may choose 000029 | \[ 000030 | \mathcal H\cong L^2(\widetilde M,S)\otimes \Hint, 000031 | \] 000032 | with $S\to\widetilde M$ the spinor bundle on the oriented double cover and $\Hint$ a finite 000033 | internal Hilbert space. This is an analytic realization choice rather than part of the boundary 000034 | datum. 000035 | \end{remark}