{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:466QCI7NH72QZYFQSTAYPNGAWD","short_pith_number":"pith:466QCI7N","schema_version":"1.0","canonical_sha256":"e7bd0123ed3ff50ce0b094c187b4c0b0cdd70608d8fd0f39a79e505ed58977e6","source":{"kind":"arxiv","id":"1911.01007","version":1},"attestation_state":"computed","paper":{"title":"Geodesic string condensation from symmetric tensor gauge theory: a unifying framework of holographic toy models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Han Yan","submitted_at":"2019-11-04T02:03:38Z","abstract_excerpt":"In this work we reason that there is a universal picture for several different holographic toy model constructions, and a gravity-like bulk field theory that gives rise it. First, we observe that the perfect tensor-networks and hyperbolic fracton models are both equivalent to the even distribution of bit-threads on geodesics in the AdS space. Such picture is also a natural \"leading-order\" approximation to the holographic entanglement properties. Then, we argue that the rank-2 U(1) theory with linearized diffeomorphism as its gauge symmetry, also known as a case of Lifshitz gravity, is the bulk"},"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":"1911.01007","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2019-11-04T02:03:38Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"9b22098cdeaf9664de14954df6147c0e8fc95d62022ec849be456ab212c6f46b","abstract_canon_sha256":"ef3e583d198daa4f33c4bd1f7ab10e8161e21c860149f5bd543d9ca96501b693"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:48:42.631936Z","signature_b64":"L0lAKotbl9KzaBJcp92LeKj0qSoI28kzjagW6TanK9nomahuCwTMbobMHbGZ4yVevzVtjbC4R+PUJAnEvjJYBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7bd0123ed3ff50ce0b094c187b4c0b0cdd70608d8fd0f39a79e505ed58977e6","last_reissued_at":"2026-07-05T01:48:42.631475Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:48:42.631475Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Geodesic string condensation from symmetric tensor gauge theory: a unifying framework of holographic toy models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Han Yan","submitted_at":"2019-11-04T02:03:38Z","abstract_excerpt":"In this work we reason that there is a universal picture for several different holographic toy model constructions, and a gravity-like bulk field theory that gives rise it. First, we observe that the perfect tensor-networks and hyperbolic fracton models are both equivalent to the even distribution of bit-threads on geodesics in the AdS space. Such picture is also a natural \"leading-order\" approximation to the holographic entanglement properties. Then, we argue that the rank-2 U(1) theory with linearized diffeomorphism as its gauge symmetry, also known as a case of Lifshitz gravity, is the bulk"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1911.01007","kind":"arxiv","version":1},"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/1911.01007/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":"1911.01007","created_at":"2026-07-05T01:48:42.631533+00:00"},{"alias_kind":"arxiv_version","alias_value":"1911.01007v1","created_at":"2026-07-05T01:48:42.631533+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1911.01007","created_at":"2026-07-05T01:48:42.631533+00:00"},{"alias_kind":"pith_short_12","alias_value":"466QCI7NH72Q","created_at":"2026-07-05T01:48:42.631533+00:00"},{"alias_kind":"pith_short_16","alias_value":"466QCI7NH72QZYFQ","created_at":"2026-07-05T01:48:42.631533+00:00"},{"alias_kind":"pith_short_8","alias_value":"466QCI7N","created_at":"2026-07-05T01:48:42.631533+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.10691","citing_title":"The thread embodiment of holographic quantum entanglement","ref_index":46,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD","json":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD.json","graph_json":"https://pith.science/api/pith-number/466QCI7NH72QZYFQSTAYPNGAWD/graph.json","events_json":"https://pith.science/api/pith-number/466QCI7NH72QZYFQSTAYPNGAWD/events.json","paper":"https://pith.science/paper/466QCI7N"},"agent_actions":{"view_html":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD","download_json":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD.json","view_paper":"https://pith.science/paper/466QCI7N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1911.01007&json=true","fetch_graph":"https://pith.science/api/pith-number/466QCI7NH72QZYFQSTAYPNGAWD/graph.json","fetch_events":"https://pith.science/api/pith-number/466QCI7NH72QZYFQSTAYPNGAWD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD/action/storage_attestation","attest_author":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD/action/author_attestation","sign_citation":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD/action/citation_signature","submit_replication":"https://pith.science/pith/466QCI7NH72QZYFQSTAYPNGAWD/action/replication_record"}},"created_at":"2026-07-05T01:48:42.631533+00:00","updated_at":"2026-07-05T01:48:42.631533+00:00"}