{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:3CSTEFKCAAUKWCB33JJIQKBTYB","short_pith_number":"pith:3CSTEFKC","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"},"canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","source":{"kind":"arxiv","id":"1706.05731","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05731","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05731v2","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05731","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"pith_short_12","alias_value":"3CSTEFKCAAUK","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3CSTEFKCAAUKWCB3","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3CSTEFKC","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:3CSTEFKCAAUKWCB33JJIQKBTYB","target":"record","payload":{"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"},"canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","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"},"source_kind":"arxiv","source_id":"1706.05731","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:22:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O1xSubaDMEX10whTuYyp+wQiJUDHJavl0vI4mr1Uy7pwg7SDML/QuXq5plSaXK++VbmPoGKA2gqH1h8b99KSBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T14:04:11.871002Z"},"content_sha256":"0e53e0fb3e18bf4df9efe7e2176bdc0372ba8f8beb22675c0a9d3d1548286cae","schema_version":"1.0","event_id":"sha256:0e53e0fb3e18bf4df9efe7e2176bdc0372ba8f8beb22675c0a9d3d1548286cae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:3CSTEFKCAAUKWCB33JJIQKBTYB","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:22:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+NG5D1MIwr3tUc5nzTwXmi+dtcQ+L7DW4a/ScuxDkYuS29suy8Fb9KV8i49eZpINCzDlWLDUlPIYBK81JEqICg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T14:04:11.871436Z"},"content_sha256":"07d40a6bbf5c18ef8c72e4fcda1c0e451d6ca9e580a35ca692494de8bb135969","schema_version":"1.0","event_id":"sha256:07d40a6bbf5c18ef8c72e4fcda1c0e451d6ca9e580a35ca692494de8bb135969"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/bundle.json","state_url":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-07T14:04:11Z","links":{"resolver":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB","bundle":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/bundle.json","state":"https://pith.science/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3CSTEFKCAAUKWCB33JJIQKBTYB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:3CSTEFKCAAUKWCB33JJIQKBTYB","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"9e24f1b8a17ac11e0af1af686aab3c566b1883dbb4cf74d05d68fdb6546b9d1b","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-18T21:52:19Z","title_canon_sha256":"93148ccf059b79fbf786c6684a038ea04782d93dc81f800cb78905ee687ae497"},"schema_version":"1.0","source":{"id":"1706.05731","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.05731","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"arxiv_version","alias_value":"1706.05731v2","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05731","created_at":"2026-05-18T00:22:29Z"},{"alias_kind":"pith_short_12","alias_value":"3CSTEFKCAAUK","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3CSTEFKCAAUKWCB3","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3CSTEFKC","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:07d40a6bbf5c18ef8c72e4fcda1c0e451d6ca9e580a35ca692494de8bb135969","target":"graph","created_at":"2026-05-18T00:22:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"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","authors_text":"Mithat \\\"Unsal, Tin Sulejmanpasic, Zohar Komargodski","cross_cats":["hep-lat","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-18T21:52:19Z","title":"Walls, Anomalies, and (De)Confinement in Quantum Anti-Ferromagnets"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05731","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0e53e0fb3e18bf4df9efe7e2176bdc0372ba8f8beb22675c0a9d3d1548286cae","target":"record","created_at":"2026-05-18T00:22:29Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"9e24f1b8a17ac11e0af1af686aab3c566b1883dbb4cf74d05d68fdb6546b9d1b","cross_cats_sorted":["hep-lat","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-06-18T21:52:19Z","title_canon_sha256":"93148ccf059b79fbf786c6684a038ea04782d93dc81f800cb78905ee687ae497"},"schema_version":"1.0","source":{"id":"1706.05731","kind":"arxiv","version":2}},"canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d8a53215420028ab083bda52882833c06335b0cd9cd49b1684907f6b5d983bc4","first_computed_at":"2026-05-18T00:22:29.066660Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:22:29.066660Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6uPI1i2U9yZ3MpUlyCVwwnz3rkTzFJ36cfEMy1vTkZCy3+0vL8E5pDtNfI00bmhAFfgi2tffk7RXV4pc3uuBBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:22:29.067500Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.05731","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0e53e0fb3e18bf4df9efe7e2176bdc0372ba8f8beb22675c0a9d3d1548286cae","sha256:07d40a6bbf5c18ef8c72e4fcda1c0e451d6ca9e580a35ca692494de8bb135969"],"state_sha256":"002178a5d9d484e3689fbe54782ac7ebff1c2928c85e8098da354d9dc7abe274"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dk/axObSqTijq1+XeWIyt/W0slzcd/L+YVztJeedHgyfqXGVZG5p8f6xC9FIZdLXspb+Vgk9dlME0ss5/2yYCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T14:04:11.873964Z","bundle_sha256":"9603de549eb4a1f208981945c0298c1021a5c41cb0ebcfb978315038e7665154"}}