← interactive companion · reference index

Results index

One row per numbered statement of the revision. Generated by tools/build_reference.py from build/free_fermion_cft_v5.aux, the manuscript as last committed on 2026-09-22; do not edit by hand, the numbers come from the compiled document and change when it is recompiled.

The new column marks the 28 statements that do not appear in free_fermion_cft_v4.tex, derived by comparing the two auxiliary files rather than asserted.

Statuses: proved in the revision, numerical where the evidence is a computation, definition and convention where nothing is claimed. The last column links to the widget on the interactive page that lets you vary the parameters.

Section 3. Scaling limits of lattice fermions

statement page what it says status new explore
Definition 3.1p. 24Convergent sequences of observables between scalesdefinition
Definition 3.2p. 25The wavelet renormalization group, built from a Daubechies scaling functiondefinitionshat
Proposition 3.3p. 26It is an inductive system; item (4) is the asymptotic compatibility that re-centring would breakproved
Definition 3.4p. 27The same maps for currents, quadratic in the fermionsdefinition
Remark 3.5p. 27Re-centring by the centre of mass, offered as a comparison convention and deliberately not built inconventionyessupport
Definition 3.6p. 28Local one-particle spaces, discarding the last 2K-1 sites of an intervaldefinition
Proposition 3.7p. 28The wavelet group preserves localisationproved
Remark 3.8p. 28A strict one-sided light cone of width eps_N(2K-1), and the linear trade-off of locality against regularityprovedyessupport
Lemma 3.9p. 29Decay of the finite products of the low-pass symbolproved
Corollary 3.10p. 30What that decay gives inside the Brillouin zone, and only thereprovedyes
Lemma 3.11p. 30Pointwise decay of the transform of the scaling functionprovedshat
Definition 3.12p. 31rho-regular means sigma_K > rho: the hypothesis the published version left as 'sufficiently regular'definitionyesladder
Remark 3.13p. 31The table of sigma_K and rho, and the four thresholds that occurnumericalyesladder
Lemma 3.14p. 32The uniform majorant: the two decays interlock across the Brillouin zoneprovedyesmajorant
Corollary 3.15p. 33The majorant in the form the dominated-convergence argument needsprovedyesmajorant
Definition 3.16p. 33The momentum-cutoff renormalization groupdefinition
Proposition 3.17p. 33It is an inductive system, and the Hardy projections leave its core invariantproved
Lemma 3.18p. 35The lattice vacua converge with no regularity hypothesis: the alias weights are probability weightsprovedalias
Corollary 3.19p. 37The scaling limit of the lattice vacua, with the rateprovedalias
Remark 3.20p. 38The massless Ramond zero mode, where the limit is convention-dependentprovedyes
Remark 3.21p. 38One argument covers both renormalization groupsproved
Remark 3.22p. 39Where the rate comes from, and why a supremum over the aliasing class would not be smallprovedyesalias

Section 4. Approximation of conformal symmetries

statement page what it says status new explore
Definition 4.1p. 40The Koo-Saleur approximantsdefinition
Remark 4.2p. 46The modified approximants' finite-scale algebra: the discrepancy vanishes for same-sign modesprovedyesdiscrepancy
Definition 4.3p. 50The one-particle Virasoro generators, renormalised: the published definition was off by L/pidefinition
Remark 4.4p. 50The central charge is 1 (resp. 1/2) for every L under this normalisationprovedyes
Corollary 4.5p. 51Analytic vectors, with radius 1/kuniform in the modeprovedradius
Remark 4.6p. 51The Majorana implementability conditionproved
Lemma 4.7p. 52Wavelet route, one particle: convergence on the whole domain, not just a coreprovedrates
Remark 4.8p. 55The sharp rate in the Sobolev scale, with a matching lower bound at the Brillouin-zone edgeprovedyesrates
Theorem 4.9p. 55Convergence of the approximants in the Fock representation (c = 0)provedrates
Corollary 4.10p. 57The one-particle Bogoliubov transformations, made quantitativeprovedduhamel
Remark 4.11p. 57The estimate for multinomials in the creation and annihilation operatorsproved
Lemma 4.12p. 57One-particle energy growth and Duhamel: linear in t at k = 0, exponential otherwiseprovedyesduhamel
Remark 4.13p. 58The same for smeared generators; the constant is sufficient but not sharpprovedyesduhamel
Corollary 4.14p. 59The derivations, with no t-dependence at allprovedduhamel
Lemma 4.15p. 60Momentum-cutoff route, one particle: the sharp rate, with no regularity of the scaling functionprovedrates
Theorem 4.16p. 61Convergence in the positive-energy representations (c = 1/2, 1). Theorem A of the introductionprovedrates
Lemma 4.17p. 62The energy bound at fixed mode, needing no regularityprovedyes
Corollary 4.18p. 62Essential self-adjointness on every core for the conformal Hamiltonian, by Nelson's commutator theoremprovedyes
Lemma 4.19p. 63Energy growth and Duhamel in Fock spaceprovedyesduhamel
Corollary 4.20p. 64The unitary groups, with a rateprovedduhamel
Corollary 4.21p. 64The Bogoliubov transformations on the momentum-cutoff routeprovedduhamel
Remark 4.22p. 64The Moebius generators in the Neveu-Schwarz sectorproved
Lemma 4.23p. 65The smeared approximants: uniform bound, domain and rateprovedrates
Remark 4.24p. 67The smearing error is a pure phase, and re-centring makes it third orderprovedyesphase
Theorem 4.25p. 68Convergence of the smeared approximants. Its rate needs K >= 7, not the K >= 6 printedprovedphase
Corollary 4.26p. 68The smeared corollaryproved
Remark 4.27p. 68Lifting the restriction to basic sequencesprovedjackson
Lemma 4.28p. 69A Jackson estimate for the loop renormalization group, driven by the total aliasing massprovedyesjackson
Theorem 4.29p. 70Reconstruction for every smooth loop, not only basic sequences; K >= 9, and K >= 10 for the rateprovedyesjackson
Remark 4.30p. 71The two-scale rateprovedyesjackson
Corollary 4.31p. 71The smeared Bogoliubov transformationsprovedduhamel
Remark 4.32p. 73The rate at nonzero mode is not an artefact of the estimatenumericalyesrates
Remark 4.33p. 74Why the supremum must be taken with care: the step Finding 1 shows to be falseprovedyesshat
Remark 4.34p. 74Simulating the theory: what the scale and the resolution mean in qubitsprovedbudget
Remark 4.35p. 75The error of the time evolution, linear in t at zero modeprovedduhamel
Remark 4.36p. 75The error for nonzero modes, on analytic vectorsprovedradius

Section 5. Approximation of Wess-Zumino-Witten currents

statement page what it says status new explore
Lemma 5.1p. 80The modified current is exact on the bulk and its off-diagonal blocks vanish identicallyprovedyescurrent
Theorem 5.2p. 80Convergence of the Wess-Zumino-Witten currents, with no regularity for the qualitative statementprovedcurrent
Remark 5.3p. 81Four ways the current is better behaved than the Virasoro generatorsprovedyescurrent

Section 6. Approximation of correlation functions

statement page what it says status new explore
Theorem 6.1p. 82Convergence of the fermion correlation functions. Theorem B of the introductionprovedbudget
Corollary 6.2p. 84The same for a wider class of observablesproved
Proposition 6.3p. 85The explicit error bound for the chiral time evolutionprovedyesbudget
Remark 6.4p. 86The end-to-end qubit budget; locality costs a square root unless one re-centresprovedyesbudget
Theorem 6.5p. 87Convergence of the Virasoro correlation functions. Theorem C, now unconditionalprovedbudget
Proposition 6.6p. 88The scale-uniform energy bound that makes Theorem C unconditionalprovedyes
Remark 6.7p. 89Mixed correlation functionsproved