Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-06-26T06:20:57.244753Z
Paper Citation Record · LEDGER
As of 22 August 2026, this Paper Citation Record lists 21 of 21 outbound references and 0 inbound Pith citation observations for arXiv:2606.23308.
A citation records a reference. It does not transfer a finding from one paper to another.
Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-06-26T06:20:57.244753Z
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-22T06:32:14.747728+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links
A source-named dated measurement, never combined with another source.
Source: cited_works
21 of 21 outbound references displayed
External citation measurements
No source-named external measurement is stored.
Observation 35546d09-53b0-4f1c-a933-0bef9b12aadd · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 1
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 2e924399-436d-41f6-8b0d-470537156290 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles The value of this gap is proportional to the real part of ∆ and is equal to 2∆ R
Reference 2
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 80368780-f9a7-4566-8848-abaddb626542 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 3
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 7bae774f-9259-4a77-b4f5-a69d1c534a5f · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles The extra electron density is n = 4x/v c, where vc =a2√ 3/ 2 is the graphene’s unit cell area
Reference 4
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 76abd33b-0426-4013-a4d7-714c3a674d0a · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Due to symmetry of the problem, the polarization operator depends only on the absolute value of the vector q
Reference 5
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 6a22f975-1471-4931-996a-a991c313fc25 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles (21) The second term in this formula includes only intra-layer interaction due to the momentum conservation low
Reference 6
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 0cd7d383-627d-40e0-90e0-e2ab4e125c28 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles For this reason, we omit the last term of Eq
Reference 7
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 794ef60d-f935-48d9-ba0b-d216652457da · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles For further consideration it is convenient to intro- duce new electronic operators, apiασ = ψ +1piασ and bpiασ = ψ − 1piασ
Reference 8
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 9069e9b9-b91d-47c3-b9f4-8bf365c28532 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 9
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation a6b0cbd6-b95b-4964-9b4b-254e1aec74dd · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles We solve these equations in the limit T → Tc
Reference 10
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation d15dc7dd-291e-43c1-8df8-4fba01e1f5b3 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles As a result, the self-consistency equation (
Reference 11
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 9e03c101-c3e5-48cc-b34f-655530763b5c · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles (28) To go further we will use the technique described, e.g., in Ref
Reference 12
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation fad9eb73-b576-4d12-8490-7b39184699e1 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 13
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 15d74fd1-c8f3-469c-96b5-fce899bb603c · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles For the reason described above we can consider both odd and even ℓ for the spin-singlet (and spin-triplet) inter- valley order parameter
Reference 14
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 6c64f561-9809-47e6-b418-ac2b1861f4fd · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles (37) From this relation, we obtain T (− ℓ) c =T (ℓ) c and ∆ (− ℓ) S1S2p = ∆ (ℓ)∗ S2S1p
Reference 15
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 51938a4f-6e32-4db8-9dd8-ca7c038d28d3 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 16
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation c010ceaa-5d29-479b-bf86-d801ff3b08e9 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Unresolved cited work
Reference 17
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation d7510f84-ca77-44f1-89ab-ec3fda79f0aa · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Thus, the most stable intra-valley state is of the spin- triplet type
Reference 18
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 0fe0469d-05ac-4ddb-ae56-1f7587283236 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Thus, the absolute values of ˜Γ (S1S2;S′ 1S′ 2) pp′ and Γ (S1S2;S′ 1S′ 2) pp′ coincide
Reference 19
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 1d62f8ea-6732-47be-977c-d181ddc1d195 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles The second term in Eq
Reference 20
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 347d29b5-c245-46be-8d2b-dd5d4d41fac9 · outbound
Kohn-Luttinger like superconductivity in twisted bilayer graphene at large twist angles Stripe Order in the Metallic and Superconducting Phases of Rhombohedral Hexalayer Graphene
Reference 21
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.
No inbound Pith citation observations are available.