{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:3CSTEFKCAAUKWCB33JJIQKBTYB","short_pith_number":"pith:3CSTEFKC","schema_version":"1.0","canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","source":{"kind":"arxiv","id":"1706.05731","version":2},"attestation_state":"computed","paper":{"title":"Walls, Anomalies, and (De)Confinement in Quantum Anti-Ferromagnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Mithat \\\"Unsal, Tin Sulejmanpasic, Zohar Komargodski","submitted_at":"2017-06-18T21:52:19Z","abstract_excerpt":"We consider the Abelian-Higgs model in 2+1 dimensions with instanton-monopole defects. This model is closely related to the phases of quantum anti-ferromagnets. In the presence of $\\mathbb{Z}_2$ preserving monopole operators, there are two confining ground states in the monopole phase, corresponding to the Valence Bond Solid (VBS) phase of quantum magnets. We show that the domain-wall carries a 't Hooft anomaly in this case. The anomaly can be saturated by, e.g., charge-conjugation breaking on the wall or by the domain wall theory becoming gapless (a gapless model that saturates the anomaly is"},"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":"1706.05731","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-18T21:52:19Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"93148ccf059b79fbf786c6684a038ea04782d93dc81f800cb78905ee687ae497","abstract_canon_sha256":"9e24f1b8a17ac11e0af1af686aab3c566b1883dbb4cf74d05d68fdb6546b9d1b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:29.067500Z","signature_b64":"6uPI1i2U9yZ3MpUlyCVwwnz3rkTzFJ36cfEMy1vTkZCy3+0vL8E5pDtNfI00bmhAFfgi2tffk7RXV4pc3uuBBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","last_reissued_at":"2026-05-18T00:22:29.066660Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:29.066660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Walls, Anomalies, and (De)Confinement in Quantum Anti-Ferromagnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Mithat \\\"Unsal, Tin Sulejmanpasic, Zohar Komargodski","submitted_at":"2017-06-18T21:52:19Z","abstract_excerpt":"We consider the Abelian-Higgs model in 2+1 dimensions with instanton-monopole defects. This model is closely related to the phases of quantum anti-ferromagnets. In the presence of $\\mathbb{Z}_2$ preserving monopole operators, there are two confining ground states in the monopole phase, corresponding to the Valence Bond Solid (VBS) phase of quantum magnets. We show that the domain-wall carries a 't Hooft anomaly in this case. The anomaly can be saturated by, e.g., charge-conjugation breaking on the wall or by the domain wall theory becoming gapless (a gapless model that saturates the anomaly is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05731","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1706.05731","created_at":"2026-05-18T00:22:29.066793+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.05731v2","created_at":"2026-05-18T00:22:29.066793+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05731","created_at":"2026-05-18T00:22:29.066793+00:00"},{"alias_kind":"pith_short_12","alias_value":"3CSTEFKCAAUK","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_16","alias_value":"3CSTEFKCAAUKWCB3","created_at":"2026-05-18T12:30:58.224056+00:00"},{"alias_kind":"pith_short_8","alias_value":"3CSTEFKC","created_at":"2026-05-18T12:30:58.224056+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2205.09545","citing_title":"Snowmass White Paper: Generalized Symmetries in Quantum Field Theory and Beyond","ref_index":289,"is_internal_anchor":true},{"citing_arxiv_id":"2605.10416","citing_title":"Infrared spectra of some strongly--coupled chiral gauge theories","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB","json":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB.json","graph_json":"https://pith.science/api/pith-number/3CSTEFKCAAUKWCB33JJIQKBTYB/graph.json","events_json":"https://pith.science/api/pith-number/3CSTEFKCAAUKWCB33JJIQKBTYB/events.json","paper":"https://pith.science/paper/3CSTEFKC"},"agent_actions":{"view_html":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB","download_json":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB.json","view_paper":"https://pith.science/paper/3CSTEFKC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.05731&json=true","fetch_graph":"https://pith.science/api/pith-number/3CSTEFKCAAUKWCB33JJIQKBTYB/graph.json","fetch_events":"https://pith.science/api/pith-number/3CSTEFKCAAUKWCB33JJIQKBTYB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/action/storage_attestation","attest_author":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/action/author_attestation","sign_citation":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/action/citation_signature","submit_replication":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/action/replication_record"}},"created_at":"2026-05-18T00:22:29.066793+00:00","updated_at":"2026-05-18T00:22:29.066793+00:00"}