{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:4ZCNAKYZCI43FNVVJ5JUIREH4J","short_pith_number":"pith:4ZCNAKYZ","schema_version":"1.0","canonical_sha256":"e644d02b191239b2b6b54f53444487e25dc9c9fd340b0b2d15bd6058d6ee85a1","source":{"kind":"arxiv","id":"hep-th/0601062","version":3},"attestation_state":"computed","paper":{"title":"Effective Dynamics of the Matrix Big Bang","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arvind Rajaraman, Ben Craps, Savdeep Sethi","submitted_at":"2006-01-10T20:14:51Z","abstract_excerpt":"We study the leading quantum effects in the recently introduced Matrix Big Bang model. This amounts to a study of supersymmetric Yang-Mills theory compactified on the Milne orbifold. We find a one-loop potential that is attractive near the Big Bang. Surprisingly, the potential decays very rapidly at late times, where it appears to be generated by D-brane effects. Usually, general covariance constrains the form of any effective action generated by renormalization group flow. However, the form of our one-loop potential seems to violate these constraints in a manner that suggests a connection bet"},"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/0601062","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-01-10T20:14:51Z","cross_cats_sorted":[],"title_canon_sha256":"4f4d1c758f214b9b4beb4a00db8d5d815b617595de286edcb8cf75266dca7207","abstract_canon_sha256":"4167a5dc97ab151df64813b074a820165034f6dcd7c578897c73c230784c8fab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:55.785144Z","signature_b64":"bzFSfgOs6oKuZ+gaE5tcaNKRNlHP8EVyqZhoKjo0DFo6xAbLb8XxlFa/F0+xBe6359gqHH0RS3aDkxMRfL11Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e644d02b191239b2b6b54f53444487e25dc9c9fd340b0b2d15bd6058d6ee85a1","last_reissued_at":"2026-07-04T15:19:55.784387Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:55.784387Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Dynamics of the Matrix Big Bang","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arvind Rajaraman, Ben Craps, Savdeep Sethi","submitted_at":"2006-01-10T20:14:51Z","abstract_excerpt":"We study the leading quantum effects in the recently introduced Matrix Big Bang model. This amounts to a study of supersymmetric Yang-Mills theory compactified on the Milne orbifold. We find a one-loop potential that is attractive near the Big Bang. Surprisingly, the potential decays very rapidly at late times, where it appears to be generated by D-brane effects. Usually, general covariance constrains the form of any effective action generated by renormalization group flow. However, the form of our one-loop potential seems to violate these constraints in a manner that suggests a connection bet"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0601062","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/0601062/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/0601062","created_at":"2026-07-04T15:19:55.784463+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0601062v3","created_at":"2026-07-04T15:19:55.784463+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0601062","created_at":"2026-07-04T15:19:55.784463+00:00"},{"alias_kind":"pith_short_12","alias_value":"4ZCNAKYZCI43","created_at":"2026-07-04T15:19:55.784463+00:00"},{"alias_kind":"pith_short_16","alias_value":"4ZCNAKYZCI43FNVV","created_at":"2026-07-04T15:19:55.784463+00:00"},{"alias_kind":"pith_short_8","alias_value":"4ZCNAKYZ","created_at":"2026-07-04T15:19:55.784463+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/4ZCNAKYZCI43FNVVJ5JUIREH4J","json":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J.json","graph_json":"https://pith.science/api/pith-number/4ZCNAKYZCI43FNVVJ5JUIREH4J/graph.json","events_json":"https://pith.science/api/pith-number/4ZCNAKYZCI43FNVVJ5JUIREH4J/events.json","paper":"https://pith.science/paper/4ZCNAKYZ"},"agent_actions":{"view_html":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J","download_json":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J.json","view_paper":"https://pith.science/paper/4ZCNAKYZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0601062&json=true","fetch_graph":"https://pith.science/api/pith-number/4ZCNAKYZCI43FNVVJ5JUIREH4J/graph.json","fetch_events":"https://pith.science/api/pith-number/4ZCNAKYZCI43FNVVJ5JUIREH4J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J/action/storage_attestation","attest_author":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J/action/author_attestation","sign_citation":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J/action/citation_signature","submit_replication":"https://pith.science/pith/4ZCNAKYZCI43FNVVJ5JUIREH4J/action/replication_record"}},"created_at":"2026-07-04T15:19:55.784463+00:00","updated_at":"2026-07-04T15:19:55.784463+00:00"}