TFPT scientific source excerpt Original repository path: tex-artefacts/toe_research_20260909.tex Original file SHA-256: 361c3843779f78c66ff7e19b610152f38d5dc4f6623ed9017c9d515f1dc94433 Inclusive original lines: 67-95 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. 000067 | Second quantization relative to the filled sea maps the target vacuum, 000068 | particles and holes into the same source Fock space. With 000069 | $a_j=b_j$ for $j\leq0$ and $a_j=d_j^*$ for $j\geq1$, the target is 000070 | \[ 000071 | H=\sum_j |j-\tfrac14|\,n_j^{\rm exc},\qquad 000072 | Q=\sum_{j\leq0}n_j^b-\sum_{j\geq1}n_j^d. 000073 | \] 000074 | The resulting contractions intertwine both field adjoints and charge in 000075 | the limit on the common finite-energy core. Orthogonality of momentum 000076 | residuals bounds the $k$-excitation generator error by $k$ times the 000077 | one-particle error, not by the $8N$ sea occupation. Since each excitation 000078 | costs at least $1/4$, $k\leq\lfloor4E\rfloor$ on an energy-$E$ core. 000079 | For $S_m=\sum_j|j-\tfrac14|^m|f_j|$ one also obtains the uniform bounds 000080 | \[ 000081 | \|\Psi_N(g)\|\leq S_0,\quad 000082 | \|[\mathcal H_N,\Psi_N(g)]\|\leq S_1,\quad 000083 | \text{time-transport error}\leq 000084 | |t|\left(\frac{\pi S_2}{N}+\frac{2\pi^2 S_3}{3N^2}\right), 000085 | \] 000086 | with transported test function 000087 | $g_t(x)=e^{it/4}g(x-t/(2\pi))$ in the source convention. 000088 | All fixed smooth finite field words and their vacuum moments follow by 000089 | bounded-product convergence. The top-edge charge-sector minima are 000090 | \[ 000091 | E_{\rm top}(q)=q^2/2-q/4,\qquad q\in\mathbb Z. 000092 | \] 000093 | They are not minima over both edges of the whole cylinder. 000094 | The microscopic holonomy term has not been removed to fit a target. 000095 | Full proof and controls: \path{microscopic-charged-car-limit/} in the archive.