Recent submissions

Comment · 6 months ago
fluorographane is a single atomic layer — one carbon thick — so storage density is naturally per unit area. The paper also gives volumetric density for the nanotape spool architecture (0.4–9 ZB/cm³, Section 4.4).
Comment · 6 months ago
The journal (Graphene, ASP) ceased operations and the DOI infrastructure went dark. The paper itself is archived at ResearchGate: researchgate.net/publication/258423577. The content is independently verifiable.
Comment · 6 months ago
The scanning-probe claim is real — C-AFM on fluorographane is achievable with existing commercial instruments. The paper is a computational prediction with a detailed experimental protocol. An experimental collaborator is preparing the validation now. The 'live conditions' question is addressed in Section 5 (radiation hardness, mechanical damage, defect physics).
Comment · 6 months ago
First PhD: algebraic cryptanalysis (Pisa). Second PhD: exact solutions to the Schrödinger equation for few-body systems (UCF). Both unrelated to fluorographane — the connection emerged later.
Comment · 6 months ago
The fluorine doesn't pass through carbon. It passes between two neighboring carbons through a C-C gap of 2.64 Å at the transition state. This is pyramidal inversion — the same mechanism as ammonia (NH₃), but with a 4.6 eV barrier instead of 0.25 eV. The transition state geometry is computed and verified with one imaginary frequency.
Comment · 6 months ago
Patent strategy is under consideration. Happy to discuss offline — [email protected].
Comment · 6 months ago
Author here. Some fair points, some misreadings.

The caching comment refers to the Tier 1 controller holding a bitmap of bits it has already scanned — standard practice in any scanning probe system. It's not competing with the storage medium for capacity.

Tier 2 is explicitly labeled speculative. The paper's validation target is Tier 1: one C-AFM scan, one voltage pulse, existing equipment.

The core contribution is not the architecture — it's the physics: a verified transition state for C-F pyramidal inversion at 4.6 eV (B3LYP) and 4.8 eV (CCSD(T)), one imaginary frequency, barrier below bond dissociation. That's standard computational chemistry, not handwaving. The architecture sections are forward-looking by design.

The fluorine passes between two carbon neighbors through a C-C gap of 2.64 Å at the transition state — not through any atom. This is pyramidal inversion, the same mechanism as ammonia, but with a 4.6 eV barrier instead of 0.25 eV.

Magnetic tape comparison is in Table 2.

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