{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:GEAIM6VPFOQMPQ4THELU6EOUQH","short_pith_number":"pith:GEAIM6VP","schema_version":"1.0","canonical_sha256":"3100867aaf2ba0c7c39339174f11d481de62d04f1df97147075fe0bf5966b8ee","source":{"kind":"arxiv","id":"2312.11096","version":2},"attestation_state":"computed","paper":{"title":"Toward higher-spin symmetry breaking in the bulk","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.V. Korybut, V.E. Didenko","submitted_at":"2023-12-18T10:47:59Z","abstract_excerpt":"We present a new vacuum of the bosonic higher-spin gauge theory in $d+1$ dimensions, which has leftover symmetry of the Poincar\\'{e} algebra in $d$ dimensions. Its structure is very simple: the space-time geometry is that of $AdS$, while the only nonzero field is a scalar. The scalar extends along the Poincar\\'{e} radial coordinate $z$ and is shown to be linearly exact for an arbitrary mixture of its two $\\Delta=2$ and $\\Delta=d-2$ conformal branches. The obtained vacuum breaks the global higher-spin symmetry leading to a broken phase that lives in the Minkowski space-time."},"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":"2312.11096","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-12-18T10:47:59Z","cross_cats_sorted":[],"title_canon_sha256":"c1cd14861914d92131706c856a8c2f45d12b191e3f880dc1eb9e332bff4c9432","abstract_canon_sha256":"7629bdf8ccdd78f0cf85f29ee861f96288dedb792722fd16c29cfe0be4305300"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:50:26.363471Z","signature_b64":"NmUfb8OuMNy0EMpGSPyy95TeSGmjziUDo2qQ2iW9EkFpz5vIMlUcQU2QnNMfQjfQ73uUsKF+0XJv/qWMrqMLBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3100867aaf2ba0c7c39339174f11d481de62d04f1df97147075fe0bf5966b8ee","last_reissued_at":"2026-07-05T08:50:26.363024Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:50:26.363024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Toward higher-spin symmetry breaking in the bulk","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.V. Korybut, V.E. Didenko","submitted_at":"2023-12-18T10:47:59Z","abstract_excerpt":"We present a new vacuum of the bosonic higher-spin gauge theory in $d+1$ dimensions, which has leftover symmetry of the Poincar\\'{e} algebra in $d$ dimensions. Its structure is very simple: the space-time geometry is that of $AdS$, while the only nonzero field is a scalar. The scalar extends along the Poincar\\'{e} radial coordinate $z$ and is shown to be linearly exact for an arbitrary mixture of its two $\\Delta=2$ and $\\Delta=d-2$ conformal branches. The obtained vacuum breaks the global higher-spin symmetry leading to a broken phase that lives in the Minkowski space-time."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.11096","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2312.11096/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":"2312.11096","created_at":"2026-07-05T08:50:26.363081+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.11096v2","created_at":"2026-07-05T08:50:26.363081+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.11096","created_at":"2026-07-05T08:50:26.363081+00:00"},{"alias_kind":"pith_short_12","alias_value":"GEAIM6VPFOQM","created_at":"2026-07-05T08:50:26.363081+00:00"},{"alias_kind":"pith_short_16","alias_value":"GEAIM6VPFOQMPQ4T","created_at":"2026-07-05T08:50:26.363081+00:00"},{"alias_kind":"pith_short_8","alias_value":"GEAIM6VP","created_at":"2026-07-05T08:50:26.363081+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.01477","citing_title":"On symmetry breaking in the self-dual higher-spin theory","ref_index":74,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH","json":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH.json","graph_json":"https://pith.science/api/pith-number/GEAIM6VPFOQMPQ4THELU6EOUQH/graph.json","events_json":"https://pith.science/api/pith-number/GEAIM6VPFOQMPQ4THELU6EOUQH/events.json","paper":"https://pith.science/paper/GEAIM6VP"},"agent_actions":{"view_html":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH","download_json":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH.json","view_paper":"https://pith.science/paper/GEAIM6VP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.11096&json=true","fetch_graph":"https://pith.science/api/pith-number/GEAIM6VPFOQMPQ4THELU6EOUQH/graph.json","fetch_events":"https://pith.science/api/pith-number/GEAIM6VPFOQMPQ4THELU6EOUQH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH/action/storage_attestation","attest_author":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH/action/author_attestation","sign_citation":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH/action/citation_signature","submit_replication":"https://pith.science/pith/GEAIM6VPFOQMPQ4THELU6EOUQH/action/replication_record"}},"created_at":"2026-07-05T08:50:26.363081+00:00","updated_at":"2026-07-05T08:50:26.363081+00:00"}