{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:QQR3AN54RH7YIGCYXH5CEUQDYA","short_pith_number":"pith:QQR3AN54","schema_version":"1.0","canonical_sha256":"8423b037bc89ff841858b9fa225203c034f08c59f4c71a3fc4ff5cb4faa2cbc5","source":{"kind":"arxiv","id":"2110.09529","version":1},"attestation_state":"computed","paper":{"title":"Anomaly Inflow for Subsystem Symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Fiona J. Burnell, Ho Tat Lam, Pranay Gorantla, Shu-Heng Shao, Trithep Devakul","submitted_at":"2021-10-18T18:00:01Z","abstract_excerpt":"We study 't Hooft anomalies and the related anomaly inflow for subsystem global symmetries. These symmetries and anomalies arise in a number of exotic systems, including models with fracton order such as the X-cube model. As is the case for ordinary global symmetries, anomalies for subsystem symmetries can be canceled by anomaly inflow from a bulk theory in one higher dimension; the corresponding bulk is therefore a non-trivial subsystem symmetry protected topological (SSPT) phase. We demonstrate these phenomena in several examples with continuous and discrete subsystem global symmetries, as w"},"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":"2110.09529","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2021-10-18T18:00:01Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b1055963e97a89c2b78a764b83c5b2d57d761db285174b96d6f9464ce434ea17","abstract_canon_sha256":"fa7d44756bd89862f1139df61816843037950ed40574860be2b3d9c21fb9e58c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:52:35.878685Z","signature_b64":"xZWr93QP8Zl8a3wvkxwMR1TUUnEsHl2Kd8vSzwg6sV1ukA/3bIoZoQfhbfyRSoyZ74EZnylMJRUf/WIAAKsOAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8423b037bc89ff841858b9fa225203c034f08c59f4c71a3fc4ff5cb4faa2cbc5","last_reissued_at":"2026-07-05T04:52:35.878209Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:52:35.878209Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomaly Inflow for Subsystem Symmetries","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Fiona J. Burnell, Ho Tat Lam, Pranay Gorantla, Shu-Heng Shao, Trithep Devakul","submitted_at":"2021-10-18T18:00:01Z","abstract_excerpt":"We study 't Hooft anomalies and the related anomaly inflow for subsystem global symmetries. These symmetries and anomalies arise in a number of exotic systems, including models with fracton order such as the X-cube model. As is the case for ordinary global symmetries, anomalies for subsystem symmetries can be canceled by anomaly inflow from a bulk theory in one higher dimension; the corresponding bulk is therefore a non-trivial subsystem symmetry protected topological (SSPT) phase. We demonstrate these phenomena in several examples with continuous and discrete subsystem global symmetries, as w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.09529","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/2110.09529/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":"2110.09529","created_at":"2026-07-05T04:52:35.878265+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.09529v1","created_at":"2026-07-05T04:52:35.878265+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.09529","created_at":"2026-07-05T04:52:35.878265+00:00"},{"alias_kind":"pith_short_12","alias_value":"QQR3AN54RH7Y","created_at":"2026-07-05T04:52:35.878265+00:00"},{"alias_kind":"pith_short_16","alias_value":"QQR3AN54RH7YIGCY","created_at":"2026-07-05T04:52:35.878265+00:00"},{"alias_kind":"pith_short_8","alias_value":"QQR3AN54","created_at":"2026-07-05T04:52:35.878265+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2504.11449","citing_title":"SymTFT construction of gapless exotic-foliated dual models","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2205.09545","citing_title":"Snowmass White Paper: Generalized Symmetries in Quantum Field Theory and Beyond","ref_index":148,"is_internal_anchor":false},{"citing_arxiv_id":"2603.19381","citing_title":"Matrix Product States for Modulated Topological Phases: Crystalline Equivalence Principle and Lieb-Schultz-Mattis Constraints","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07293","citing_title":"Exotic theta terms in 2+1d fractonic field theory","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA","json":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA.json","graph_json":"https://pith.science/api/pith-number/QQR3AN54RH7YIGCYXH5CEUQDYA/graph.json","events_json":"https://pith.science/api/pith-number/QQR3AN54RH7YIGCYXH5CEUQDYA/events.json","paper":"https://pith.science/paper/QQR3AN54"},"agent_actions":{"view_html":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA","download_json":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA.json","view_paper":"https://pith.science/paper/QQR3AN54","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.09529&json=true","fetch_graph":"https://pith.science/api/pith-number/QQR3AN54RH7YIGCYXH5CEUQDYA/graph.json","fetch_events":"https://pith.science/api/pith-number/QQR3AN54RH7YIGCYXH5CEUQDYA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA/action/storage_attestation","attest_author":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA/action/author_attestation","sign_citation":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA/action/citation_signature","submit_replication":"https://pith.science/pith/QQR3AN54RH7YIGCYXH5CEUQDYA/action/replication_record"}},"created_at":"2026-07-05T04:52:35.878265+00:00","updated_at":"2026-07-05T04:52:35.878265+00:00"}