{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:ICS5QHUXUFOQGSGFILTVNJ7BH7","short_pith_number":"pith:ICS5QHUX","schema_version":"1.0","canonical_sha256":"40a5d81e97a15d0348c542e756a7e13fe4f97ac62ffe90440394be4e53c184e0","source":{"kind":"arxiv","id":"hep-th/9902155","version":3},"attestation_state":"computed","paper":{"title":"Dilaton-driven confinement","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Steven S. Gubser (Harvard)","submitted_at":"1999-02-22T22:58:03Z","abstract_excerpt":"We derive a solution of type IIB supergravity which is asymptotic to AdS_5 x S^5, has SO(6) symmetry, and exhibits some of the features expected of geometries dual to confining gauge theories. At the linearized level, the solution differs from pure AdS_5 x S^5 only by a dilaton profile. It has a naked singularity in the interior. Wilson loops follow area law behavior, and there is a mass gap. We suggest a field theory interpretation in which all matter fields of N=4 gauge theory acquire a mass and the infrared theory is confining."},"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":"hep-th/9902155","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-02-22T22:58:03Z","cross_cats_sorted":[],"title_canon_sha256":"b5257983774fbedc8ec3ccc96fa4c3e5a5a05e76b1bb323d515cfcbba977f953","abstract_canon_sha256":"7b779f7d34c3e7d5f9dce0e56d46748dfe0e93992a2a34b757f32e3d76c7f21c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:33:20.357736Z","signature_b64":"c/iKjLi7iNo8gpYBE5SuX1oNzi57TrJE5wpoKXKth0IO4dgS/V4ACnWD47dBhl4f0A0heMKFb8GP+gSaRxUJBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40a5d81e97a15d0348c542e756a7e13fe4f97ac62ffe90440394be4e53c184e0","last_reissued_at":"2026-07-04T14:33:20.357385Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:33:20.357385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dilaton-driven confinement","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Steven S. Gubser (Harvard)","submitted_at":"1999-02-22T22:58:03Z","abstract_excerpt":"We derive a solution of type IIB supergravity which is asymptotic to AdS_5 x S^5, has SO(6) symmetry, and exhibits some of the features expected of geometries dual to confining gauge theories. At the linearized level, the solution differs from pure AdS_5 x S^5 only by a dilaton profile. It has a naked singularity in the interior. Wilson loops follow area law behavior, and there is a mass gap. We suggest a field theory interpretation in which all matter fields of N=4 gauge theory acquire a mass and the infrared theory is confining."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9902155","kind":"arxiv","version":3},"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/hep-th/9902155/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":"hep-th/9902155","created_at":"2026-07-04T14:33:20.357437+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9902155v3","created_at":"2026-07-04T14:33:20.357437+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9902155","created_at":"2026-07-04T14:33:20.357437+00:00"},{"alias_kind":"pith_short_12","alias_value":"ICS5QHUXUFOQ","created_at":"2026-07-04T14:33:20.357437+00:00"},{"alias_kind":"pith_short_16","alias_value":"ICS5QHUXUFOQGSGF","created_at":"2026-07-04T14:33:20.357437+00:00"},{"alias_kind":"pith_short_8","alias_value":"ICS5QHUX","created_at":"2026-07-04T14:33:20.357437+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2511.18128","citing_title":"Supersymmetric AdS Solitons, Coulomb Branch Flows and Twisted Compactifications","ref_index":68,"is_internal_anchor":true},{"citing_arxiv_id":"2512.02484","citing_title":"Properties of Stable Massive Quark Stars in Holography","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7","json":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7.json","graph_json":"https://pith.science/api/pith-number/ICS5QHUXUFOQGSGFILTVNJ7BH7/graph.json","events_json":"https://pith.science/api/pith-number/ICS5QHUXUFOQGSGFILTVNJ7BH7/events.json","paper":"https://pith.science/paper/ICS5QHUX"},"agent_actions":{"view_html":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7","download_json":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7.json","view_paper":"https://pith.science/paper/ICS5QHUX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9902155&json=true","fetch_graph":"https://pith.science/api/pith-number/ICS5QHUXUFOQGSGFILTVNJ7BH7/graph.json","fetch_events":"https://pith.science/api/pith-number/ICS5QHUXUFOQGSGFILTVNJ7BH7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7/action/storage_attestation","attest_author":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7/action/author_attestation","sign_citation":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7/action/citation_signature","submit_replication":"https://pith.science/pith/ICS5QHUXUFOQGSGFILTVNJ7BH7/action/replication_record"}},"created_at":"2026-07-04T14:33:20.357437+00:00","updated_at":"2026-07-04T14:33:20.357437+00:00"}