{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:6TYZ3JCVFZX4ZJTPTKTIH7VWPQ","short_pith_number":"pith:6TYZ3JCV","schema_version":"1.0","canonical_sha256":"f4f19da4552e6fcca66f9aa683feb67c20419dc8b4e4acf36e4c65eab12e1619","source":{"kind":"arxiv","id":"hep-th/0009156","version":3},"attestation_state":"computed","paper":{"title":"Anatomy of Two Holographic Renormalization Group Flows","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Z. Freedman, Krzysztof Pilch, Massimo Bianchi, Oliver DeWolfe","submitted_at":"2000-09-20T18:41:44Z","abstract_excerpt":"We derive and solve a subset of the fluctuation equations about two domain wall solutions of D=5, N=8 gauged supergravity. One solution is dual to D=4, N=4 SYM theory perturbed by an N=1, SO(3)-invariant mass term and the other to a Coulomb branch deformation. In the first case we study all SO(3)-singlet fields. These are assembled into bulk multiplets dual to the stress tensor multiplet and to the N=1 chiral multiplets Tr Phi^2 and Tr W^2, the former playing the role of anomaly multiplet. Each of these three multiplets has a distinct spectrum of \"glueball\" states. This behavior is contrasted "},"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/0009156","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2000-09-20T18:41:44Z","cross_cats_sorted":[],"title_canon_sha256":"6a98f509d4df4c182fdf87a9d5713db3ad70624c9cd201d742ac3ee7d78b7f50","abstract_canon_sha256":"a0d0ce0ead9580b9718734b91a24a3d5b49e9bd460bc32a5c9e586a1b467740a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:21:02.529372Z","signature_b64":"Yyu9leT+XS1UyjP5iEyWdibI9PHwIJmkpxwE3kwijxYDfYENxNWFUvU7T4IHf6E9HruKuVD8Vgf7hv0eRouBCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4f19da4552e6fcca66f9aa683feb67c20419dc8b4e4acf36e4c65eab12e1619","last_reissued_at":"2026-07-04T16:21:02.528828Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:21:02.528828Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anatomy of Two Holographic Renormalization Group Flows","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Z. Freedman, Krzysztof Pilch, Massimo Bianchi, Oliver DeWolfe","submitted_at":"2000-09-20T18:41:44Z","abstract_excerpt":"We derive and solve a subset of the fluctuation equations about two domain wall solutions of D=5, N=8 gauged supergravity. One solution is dual to D=4, N=4 SYM theory perturbed by an N=1, SO(3)-invariant mass term and the other to a Coulomb branch deformation. In the first case we study all SO(3)-singlet fields. These are assembled into bulk multiplets dual to the stress tensor multiplet and to the N=1 chiral multiplets Tr Phi^2 and Tr W^2, the former playing the role of anomaly multiplet. Each of these three multiplets has a distinct spectrum of \"glueball\" states. This behavior is contrasted "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0009156","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/0009156/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/0009156","created_at":"2026-07-04T16:21:02.528885+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0009156v3","created_at":"2026-07-04T16:21:02.528885+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0009156","created_at":"2026-07-04T16:21:02.528885+00:00"},{"alias_kind":"pith_short_12","alias_value":"6TYZ3JCVFZX4","created_at":"2026-07-04T16:21:02.528885+00:00"},{"alias_kind":"pith_short_16","alias_value":"6TYZ3JCVFZX4ZJTP","created_at":"2026-07-04T16:21:02.528885+00:00"},{"alias_kind":"pith_short_8","alias_value":"6TYZ3JCV","created_at":"2026-07-04T16:21:02.528885+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":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ","json":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ.json","graph_json":"https://pith.science/api/pith-number/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/graph.json","events_json":"https://pith.science/api/pith-number/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/events.json","paper":"https://pith.science/paper/6TYZ3JCV"},"agent_actions":{"view_html":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ","download_json":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ.json","view_paper":"https://pith.science/paper/6TYZ3JCV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0009156&json=true","fetch_graph":"https://pith.science/api/pith-number/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/graph.json","fetch_events":"https://pith.science/api/pith-number/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/action/storage_attestation","attest_author":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/action/author_attestation","sign_citation":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/action/citation_signature","submit_replication":"https://pith.science/pith/6TYZ3JCVFZX4ZJTPTKTIH7VWPQ/action/replication_record"}},"created_at":"2026-07-04T16:21:02.528885+00:00","updated_at":"2026-07-04T16:21:02.528885+00:00"}