{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:7SBVWDUUO6BMACFAKB73FD5F56","short_pith_number":"pith:7SBVWDUU","schema_version":"1.0","canonical_sha256":"fc835b0e947782c008a0507fb28fa5ef8ef3feeb0dff8fdfd8de934a21b9f854","source":{"kind":"arxiv","id":"hep-th/0107167","version":2},"attestation_state":"computed","paper":{"title":"A Remark on Non-conformal Non-supersymmetric Theories with Vanishing Vacuum Energy Density","license":"","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Alberto Iglesias, Olindo Corradini, Peter Langfelder, Zurab Kakushadze","submitted_at":"2001-07-20T00:14:14Z","abstract_excerpt":"We discuss non-conformal non-supersymmetric large N gauge theories with vanishing vacuum energy density to all orders in perturbation theory. These gauge theories can be obtained via a field theory limit of Type IIB D3-branes embedded in orbifolded space-times. We also discuss gravity in this setup."},"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/0107167","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2001-07-20T00:14:14Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"05801a1759e9249b48833fba54fcf2b3c0513f635eddabe12d265046b649b316","abstract_canon_sha256":"211219a98df48de1041284b3931752882cdea1162bf5820211effe9b302bd567"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:11.826903Z","signature_b64":"Df07v0MAi/xZ1UY07tmuWHnxxYKUVcibyD6DjjZDW71jCMQytyRaN1PDZSqjv9Em1jpnQErQMIBWYkMhtFzXCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc835b0e947782c008a0507fb28fa5ef8ef3feeb0dff8fdfd8de934a21b9f854","last_reissued_at":"2026-05-18T02:36:11.826479Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:11.826479Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Remark on Non-conformal Non-supersymmetric Theories with Vanishing Vacuum Energy Density","license":"","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"Alberto Iglesias, Olindo Corradini, Peter Langfelder, Zurab Kakushadze","submitted_at":"2001-07-20T00:14:14Z","abstract_excerpt":"We discuss non-conformal non-supersymmetric large N gauge theories with vanishing vacuum energy density to all orders in perturbation theory. These gauge theories can be obtained via a field theory limit of Type IIB D3-branes embedded in orbifolded space-times. We also discuss gravity in this setup."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0107167","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":""},"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/0107167","created_at":"2026-05-18T02:36:11.826537+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0107167v2","created_at":"2026-05-18T02:36:11.826537+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0107167","created_at":"2026-05-18T02:36:11.826537+00:00"},{"alias_kind":"pith_short_12","alias_value":"7SBVWDUUO6BM","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"7SBVWDUUO6BMACFA","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"7SBVWDUU","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56","json":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56.json","graph_json":"https://pith.science/api/pith-number/7SBVWDUUO6BMACFAKB73FD5F56/graph.json","events_json":"https://pith.science/api/pith-number/7SBVWDUUO6BMACFAKB73FD5F56/events.json","paper":"https://pith.science/paper/7SBVWDUU"},"agent_actions":{"view_html":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56","download_json":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56.json","view_paper":"https://pith.science/paper/7SBVWDUU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0107167&json=true","fetch_graph":"https://pith.science/api/pith-number/7SBVWDUUO6BMACFAKB73FD5F56/graph.json","fetch_events":"https://pith.science/api/pith-number/7SBVWDUUO6BMACFAKB73FD5F56/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56/action/storage_attestation","attest_author":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56/action/author_attestation","sign_citation":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56/action/citation_signature","submit_replication":"https://pith.science/pith/7SBVWDUUO6BMACFAKB73FD5F56/action/replication_record"}},"created_at":"2026-05-18T02:36:11.826537+00:00","updated_at":"2026-05-18T02:36:11.826537+00:00"}