{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:SU3RM6E3MKEM4STEJ7U6EKJBZY","short_pith_number":"pith:SU3RM6E3","schema_version":"1.0","canonical_sha256":"953716789b6288ce4a644fe9e22921ce15b9e117f38e04de482895b17a2fdb1b","source":{"kind":"arxiv","id":"2405.06515","version":2},"attestation_state":"computed","paper":{"title":"Holographic RG flows in a 3d gauged supergravity at finite temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alexander Nikolaev, Anastasia Golubtsova, Mikhail Podoinitsyn","submitted_at":"2024-05-10T14:54:11Z","abstract_excerpt":"In this paper we consider finite-temperature holographic RG flows in $D=3$ $\\mathcal{N}=(2,0)$ gauged truncated supergravity coupled to a sigma model with a hyperbolic target space. In the context of the holographic duality, fixed points (CFTs) at finite temperature are described by AdS black holes. We come from the gravity EOM to a 3d autonomous dynamical system, which critical points can be related to fixed points of dual field theories. Near-horizon black hole solutions correspond to infinite points of this system. We use Poincar\\'e transformations to project the system on $\\mathbf{R}^3$ in"},"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":"2405.06515","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-05-10T14:54:11Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"4d6e644488345a4974f445e8ee14f5a0b4d04fb493d4bb8dfd64fb9d16c277ff","abstract_canon_sha256":"5a6f71ab0a6e83850b9842c2f640962d1c83f6b637f2aa772ed240634dd48b79"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:31:15.260711Z","signature_b64":"HpjexDdkiaaJKMpXRB8SOLZqzspsOJMWTZyuapKHwIZ7U56jKmrqvWq08PjqBvtb1bI+++3PjuyS8Q37KfmEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"953716789b6288ce4a644fe9e22921ce15b9e117f38e04de482895b17a2fdb1b","last_reissued_at":"2026-07-05T08:31:15.260226Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:31:15.260226Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Holographic RG flows in a 3d gauged supergravity at finite temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alexander Nikolaev, Anastasia Golubtsova, Mikhail Podoinitsyn","submitted_at":"2024-05-10T14:54:11Z","abstract_excerpt":"In this paper we consider finite-temperature holographic RG flows in $D=3$ $\\mathcal{N}=(2,0)$ gauged truncated supergravity coupled to a sigma model with a hyperbolic target space. In the context of the holographic duality, fixed points (CFTs) at finite temperature are described by AdS black holes. We come from the gravity EOM to a 3d autonomous dynamical system, which critical points can be related to fixed points of dual field theories. Near-horizon black hole solutions correspond to infinite points of this system. We use Poincar\\'e transformations to project the system on $\\mathbf{R}^3$ in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.06515","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/2405.06515/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":"2405.06515","created_at":"2026-07-05T08:31:15.260281+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.06515v2","created_at":"2026-07-05T08:31:15.260281+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.06515","created_at":"2026-07-05T08:31:15.260281+00:00"},{"alias_kind":"pith_short_12","alias_value":"SU3RM6E3MKEM","created_at":"2026-07-05T08:31:15.260281+00:00"},{"alias_kind":"pith_short_16","alias_value":"SU3RM6E3MKEM4STE","created_at":"2026-07-05T08:31:15.260281+00:00"},{"alias_kind":"pith_short_8","alias_value":"SU3RM6E3","created_at":"2026-07-05T08:31:15.260281+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.16749","citing_title":"Janus and RG-interfaces in minimal 3d gauged supergravity","ref_index":41,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY","json":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY.json","graph_json":"https://pith.science/api/pith-number/SU3RM6E3MKEM4STEJ7U6EKJBZY/graph.json","events_json":"https://pith.science/api/pith-number/SU3RM6E3MKEM4STEJ7U6EKJBZY/events.json","paper":"https://pith.science/paper/SU3RM6E3"},"agent_actions":{"view_html":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY","download_json":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY.json","view_paper":"https://pith.science/paper/SU3RM6E3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.06515&json=true","fetch_graph":"https://pith.science/api/pith-number/SU3RM6E3MKEM4STEJ7U6EKJBZY/graph.json","fetch_events":"https://pith.science/api/pith-number/SU3RM6E3MKEM4STEJ7U6EKJBZY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY/action/storage_attestation","attest_author":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY/action/author_attestation","sign_citation":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY/action/citation_signature","submit_replication":"https://pith.science/pith/SU3RM6E3MKEM4STEJ7U6EKJBZY/action/replication_record"}},"created_at":"2026-07-05T08:31:15.260281+00:00","updated_at":"2026-07-05T08:31:15.260281+00:00"}