{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:2HXCW676KUIUSKNM7SJQMCTYOF","short_pith_number":"pith:2HXCW676","schema_version":"1.0","canonical_sha256":"d1ee2b7bfe55114929acfc93060a787152716fd99bc332faa7b2fb811e725d80","source":{"kind":"arxiv","id":"2410.15395","version":3},"attestation_state":"computed","paper":{"title":"Topological edge states at Floquet quantum criticality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Jiangbin Gong, Longwen Zhou, Xue-Jia Yu","submitted_at":"2024-10-20T14:06:02Z","abstract_excerpt":"Topologically protected edge states exactly at topological phase boundaries challenge the conventional belief that topological states must be associated with a bulk energy gap. Because periodically driven (Floquet) systems host unusually intricate topological phase boundaries, topological edge states can be prolific at such Floquet quantum criticality. Working on a class of chiral-symmetric, Floquet-driven Majorana fermion chains, we analytically and computationally show that the precise boundaries between different Floquet topological gapped phases can accommodate topological edge modes, incl"},"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":"2410.15395","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2024-10-20T14:06:02Z","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","quant-ph"],"title_canon_sha256":"2a667a1b80b4e8150d4f1d7068667a1db109ec4f94fe16f1463619d5b7dbaa8a","abstract_canon_sha256":"43b8a732d1488cc3fa63ddce155ea9bbe4d499db72a591183b8cc09412a78c7c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:08:01.861528Z","signature_b64":"qQndWvtfMrYWhXRxFhm3rxPsB2NlnYd3klEtZVAmru+eRXR4yniLXi8jfP1tSyWme7LXTC87MGadiLaGUfegAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d1ee2b7bfe55114929acfc93060a787152716fd99bc332faa7b2fb811e725d80","last_reissued_at":"2026-07-05T11:08:01.861018Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:08:01.861018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Topological edge states at Floquet quantum criticality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Jiangbin Gong, Longwen Zhou, Xue-Jia Yu","submitted_at":"2024-10-20T14:06:02Z","abstract_excerpt":"Topologically protected edge states exactly at topological phase boundaries challenge the conventional belief that topological states must be associated with a bulk energy gap. Because periodically driven (Floquet) systems host unusually intricate topological phase boundaries, topological edge states can be prolific at such Floquet quantum criticality. Working on a class of chiral-symmetric, Floquet-driven Majorana fermion chains, we analytically and computationally show that the precise boundaries between different Floquet topological gapped phases can accommodate topological edge modes, incl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.15395","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/2410.15395/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":"2410.15395","created_at":"2026-07-05T11:08:01.861075+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.15395v3","created_at":"2026-07-05T11:08:01.861075+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.15395","created_at":"2026-07-05T11:08:01.861075+00:00"},{"alias_kind":"pith_short_12","alias_value":"2HXCW676KUIU","created_at":"2026-07-05T11:08:01.861075+00:00"},{"alias_kind":"pith_short_16","alias_value":"2HXCW676KUIUSKNM","created_at":"2026-07-05T11:08:01.861075+00:00"},{"alias_kind":"pith_short_8","alias_value":"2HXCW676","created_at":"2026-07-05T11:08:01.861075+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2501.03851","citing_title":"Gapless Symmetry-Protected Topological States in Measurement-Only Circuits","ref_index":89,"is_internal_anchor":false},{"citing_arxiv_id":"2503.01198","citing_title":"Deconfined criticality as intrinsically gapless topological state in one dimension","ref_index":118,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF","json":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF.json","graph_json":"https://pith.science/api/pith-number/2HXCW676KUIUSKNM7SJQMCTYOF/graph.json","events_json":"https://pith.science/api/pith-number/2HXCW676KUIUSKNM7SJQMCTYOF/events.json","paper":"https://pith.science/paper/2HXCW676"},"agent_actions":{"view_html":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF","download_json":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF.json","view_paper":"https://pith.science/paper/2HXCW676","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.15395&json=true","fetch_graph":"https://pith.science/api/pith-number/2HXCW676KUIUSKNM7SJQMCTYOF/graph.json","fetch_events":"https://pith.science/api/pith-number/2HXCW676KUIUSKNM7SJQMCTYOF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF/action/storage_attestation","attest_author":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF/action/author_attestation","sign_citation":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF/action/citation_signature","submit_replication":"https://pith.science/pith/2HXCW676KUIUSKNM7SJQMCTYOF/action/replication_record"}},"created_at":"2026-07-05T11:08:01.861075+00:00","updated_at":"2026-07-05T11:08:01.861075+00:00"}