{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:CGGV3VRGVOOCQ73YUO3AHJUXUT","short_pith_number":"pith:CGGV3VRG","schema_version":"1.0","canonical_sha256":"118d5dd626ab9c287f78a3b603a697a4f373c629dcea3f9c2ae76c1edfe9a6a1","source":{"kind":"arxiv","id":"2005.06561","version":1},"attestation_state":"computed","paper":{"title":"$M$-strings and AdS$_3$ solutions to M-theory with small $\\mathcal{N}=(0,4)$ supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anayeli Ramirez, Carlos Nunez, Stefano Speziali, Yolanda Lozano","submitted_at":"2020-05-13T19:52:40Z","abstract_excerpt":"We construct a general class of (small) $\\mathcal{N}=(0,4)$ superconformal solutions in M-theory of the form AdS$_3\\times S^3/\\mathbb{Z}_k\\times \\text{CY}_2$, foliated over an interval. These solutions describe M-strings in M5-brane intersections. The $M$-strings support $(0,4)$ quiver CFTs that are in correspondence with our backgrounds. We compute the central charge and show that it scales linearly with the total number of $M$-strings. We introduce momentum charge, thus allowing for a description in terms of M(atrix) theory. Upon reduction to Type IIA, we find a new class of solutions with f"},"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":"2005.06561","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-05-13T19:52:40Z","cross_cats_sorted":[],"title_canon_sha256":"d76679ae1e93e01b0d428685e86af6507e31e390777c96568ec99b87ddbb8ea6","abstract_canon_sha256":"302aca41320350c160edc95e1cf8ade8f1c5b6360af051c6d4637afd7e520daa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:02:47.919597Z","signature_b64":"EnSUDywCg1Mis+GoR/JMi+j9auQz5NOG1s1rSQsmsNlaFMKIpKoXAmTJd0YrL2o2PAiEKcFQt5DDsAhn8M/bDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"118d5dd626ab9c287f78a3b603a697a4f373c629dcea3f9c2ae76c1edfe9a6a1","last_reissued_at":"2026-07-05T01:02:47.919123Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:02:47.919123Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$M$-strings and AdS$_3$ solutions to M-theory with small $\\mathcal{N}=(0,4)$ supersymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anayeli Ramirez, Carlos Nunez, Stefano Speziali, Yolanda Lozano","submitted_at":"2020-05-13T19:52:40Z","abstract_excerpt":"We construct a general class of (small) $\\mathcal{N}=(0,4)$ superconformal solutions in M-theory of the form AdS$_3\\times S^3/\\mathbb{Z}_k\\times \\text{CY}_2$, foliated over an interval. These solutions describe M-strings in M5-brane intersections. The $M$-strings support $(0,4)$ quiver CFTs that are in correspondence with our backgrounds. We compute the central charge and show that it scales linearly with the total number of $M$-strings. We introduce momentum charge, thus allowing for a description in terms of M(atrix) theory. Upon reduction to Type IIA, we find a new class of solutions with f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2005.06561","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/2005.06561/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":"2005.06561","created_at":"2026-07-05T01:02:47.919177+00:00"},{"alias_kind":"arxiv_version","alias_value":"2005.06561v1","created_at":"2026-07-05T01:02:47.919177+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2005.06561","created_at":"2026-07-05T01:02:47.919177+00:00"},{"alias_kind":"pith_short_12","alias_value":"CGGV3VRGVOOC","created_at":"2026-07-05T01:02:47.919177+00:00"},{"alias_kind":"pith_short_16","alias_value":"CGGV3VRGVOOCQ73Y","created_at":"2026-07-05T01:02:47.919177+00:00"},{"alias_kind":"pith_short_8","alias_value":"CGGV3VRG","created_at":"2026-07-05T01:02:47.919177+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.18942","citing_title":"Covariant unification of holographic c-functions","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07432","citing_title":"Holographic Krylov Complexity for Charged, Composite and Extended Probes","ref_index":41,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT","json":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT.json","graph_json":"https://pith.science/api/pith-number/CGGV3VRGVOOCQ73YUO3AHJUXUT/graph.json","events_json":"https://pith.science/api/pith-number/CGGV3VRGVOOCQ73YUO3AHJUXUT/events.json","paper":"https://pith.science/paper/CGGV3VRG"},"agent_actions":{"view_html":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT","download_json":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT.json","view_paper":"https://pith.science/paper/CGGV3VRG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2005.06561&json=true","fetch_graph":"https://pith.science/api/pith-number/CGGV3VRGVOOCQ73YUO3AHJUXUT/graph.json","fetch_events":"https://pith.science/api/pith-number/CGGV3VRGVOOCQ73YUO3AHJUXUT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT/action/storage_attestation","attest_author":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT/action/author_attestation","sign_citation":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT/action/citation_signature","submit_replication":"https://pith.science/pith/CGGV3VRGVOOCQ73YUO3AHJUXUT/action/replication_record"}},"created_at":"2026-07-05T01:02:47.919177+00:00","updated_at":"2026-07-05T01:02:47.919177+00:00"}