{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:TCOZFWEMYS6G6TOGWKBRUILIV4","short_pith_number":"pith:TCOZFWEM","schema_version":"1.0","canonical_sha256":"989d92d88cc4bc6f4dc6b2831a2168af0c12900bfcc158ae3316423fe40a0750","source":{"kind":"arxiv","id":"2508.13571","version":3},"attestation_state":"computed","paper":{"title":"Realization and characterization of an all-bands-flat electrical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexei Andreanov, L.Q. English, Noah Lape, P.G. Kevrekidis, Sergej Flach, Simon Diubenkov, Yeongjun Kim","submitted_at":"2025-08-19T07:02:25Z","abstract_excerpt":"We construct an electrical all-bands-flat (ABF) lattice and experimentally generate compact localized states (CLSs) therein. The lattice is a diamond (rhombic) chain and implemented as a network of capacitors and inductors, as well as voltage inverters (using operational amplifiers) in order to introduce a \\(\\pi\\)-phase flux within each diamond. The network's normal modes split into three flat bands, and the corresponding CLSs can be excited in isolation via a two-node driving at the flat band frequencies. We also examine the role of the lattice edges and their interaction with the CLSs. Final"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2508.13571","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-08-19T07:02:25Z","cross_cats_sorted":["nlin.PS"],"title_canon_sha256":"01cddcbe3d8555fe7073a8f108971136d59e68feee263c7f51fadfb00b862692","abstract_canon_sha256":"0dd1d7d526b0c38fd2e79963c5b370090bfee6b0805e460b50dd032d4cd3a2bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:02:50.287701Z","signature_b64":"kJABGifVYj9snpm6IlshCgmsAcWCauvz0J8/vMRD68ZF2g/9HgVQOZl4VgGU4qybJQvE3p9vw10wnn9vbwGUAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"989d92d88cc4bc6f4dc6b2831a2168af0c12900bfcc158ae3316423fe40a0750","last_reissued_at":"2026-07-05T12:02:50.287155Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:02:50.287155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Realization and characterization of an all-bands-flat electrical lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.PS"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexei Andreanov, L.Q. English, Noah Lape, P.G. Kevrekidis, Sergej Flach, Simon Diubenkov, Yeongjun Kim","submitted_at":"2025-08-19T07:02:25Z","abstract_excerpt":"We construct an electrical all-bands-flat (ABF) lattice and experimentally generate compact localized states (CLSs) therein. The lattice is a diamond (rhombic) chain and implemented as a network of capacitors and inductors, as well as voltage inverters (using operational amplifiers) in order to introduce a \\(\\pi\\)-phase flux within each diamond. The network's normal modes split into three flat bands, and the corresponding CLSs can be excited in isolation via a two-node driving at the flat band frequencies. We also examine the role of the lattice edges and their interaction with the CLSs. Final"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.13571","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2508.13571/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2508.13571","created_at":"2026-07-05T12:02:50.287214+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.13571v3","created_at":"2026-07-05T12:02:50.287214+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.13571","created_at":"2026-07-05T12:02:50.287214+00:00"},{"alias_kind":"pith_short_12","alias_value":"TCOZFWEMYS6G","created_at":"2026-07-05T12:02:50.287214+00:00"},{"alias_kind":"pith_short_16","alias_value":"TCOZFWEMYS6G6TOG","created_at":"2026-07-05T12:02:50.287214+00:00"},{"alias_kind":"pith_short_8","alias_value":"TCOZFWEM","created_at":"2026-07-05T12:02:50.287214+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2510.17258","citing_title":"Real space decay of flat band projectors from compact localized states","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05258","citing_title":"Nematic Phase Transitions and Density Modulations in 1D Flat Band Condensates","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4","json":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4.json","graph_json":"https://pith.science/api/pith-number/TCOZFWEMYS6G6TOGWKBRUILIV4/graph.json","events_json":"https://pith.science/api/pith-number/TCOZFWEMYS6G6TOGWKBRUILIV4/events.json","paper":"https://pith.science/paper/TCOZFWEM"},"agent_actions":{"view_html":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4","download_json":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4.json","view_paper":"https://pith.science/paper/TCOZFWEM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.13571&json=true","fetch_graph":"https://pith.science/api/pith-number/TCOZFWEMYS6G6TOGWKBRUILIV4/graph.json","fetch_events":"https://pith.science/api/pith-number/TCOZFWEMYS6G6TOGWKBRUILIV4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4/action/storage_attestation","attest_author":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4/action/author_attestation","sign_citation":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4/action/citation_signature","submit_replication":"https://pith.science/pith/TCOZFWEMYS6G6TOGWKBRUILIV4/action/replication_record"}},"created_at":"2026-07-05T12:02:50.287214+00:00","updated_at":"2026-07-05T12:02:50.287214+00:00"}