{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:V4JNSDQDY3ME4P7VPFKBLCZSAY","short_pith_number":"pith:V4JNSDQD","schema_version":"1.0","canonical_sha256":"af12d90e03c6d84e3ff57954158b3206215d35cd5a818d5b003c20fae6233cc2","source":{"kind":"arxiv","id":"1508.03413","version":1},"attestation_state":"computed","paper":{"title":"Divergences and Boundary Modes in N=8 Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Finn Larsen, Pedro Lisbao","submitted_at":"2015-08-14T03:52:53Z","abstract_excerpt":"We reconsider the one loop divergence of ${\\cal N}=8$ supergravity in four dimensions. We compute the finite effective potential of ${\\cal N}=8$ anti-deSitter supergravity and interpret it as logarithmic running of the cosmological constant. We find that quantum inequivalence between fields that are classically dual is due to boundary modes in AdS$_4$. Some subtleties are traced to the difference between the Euler characteristic of global and thermal AdS$_4$."},"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":"1508.03413","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-08-14T03:52:53Z","cross_cats_sorted":[],"title_canon_sha256":"1d10ef04bd5f4080e0daf5409afcead51cb6a09f8ced0f2f5252c36155a5a885","abstract_canon_sha256":"9057e8cccaa55693f8118c49714acf7e7bafbb2ffa2406ca8165a5f5af9a2951"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:34.578935Z","signature_b64":"SiYOx8K9j+i2S+qmy8eM2k/9EjvVNLu/QdDU8fToYCU4ybRnE1tf5THcojnGDmo4oZnmj3Fsq3nSbc6zlMD4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af12d90e03c6d84e3ff57954158b3206215d35cd5a818d5b003c20fae6233cc2","last_reissued_at":"2026-05-18T01:20:34.578489Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:34.578489Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Divergences and Boundary Modes in N=8 Supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Finn Larsen, Pedro Lisbao","submitted_at":"2015-08-14T03:52:53Z","abstract_excerpt":"We reconsider the one loop divergence of ${\\cal N}=8$ supergravity in four dimensions. We compute the finite effective potential of ${\\cal N}=8$ anti-deSitter supergravity and interpret it as logarithmic running of the cosmological constant. We find that quantum inequivalence between fields that are classically dual is due to boundary modes in AdS$_4$. Some subtleties are traced to the difference between the Euler characteristic of global and thermal AdS$_4$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.03413","kind":"arxiv","version":1},"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":"1508.03413","created_at":"2026-05-18T01:20:34.578546+00:00"},{"alias_kind":"arxiv_version","alias_value":"1508.03413v1","created_at":"2026-05-18T01:20:34.578546+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.03413","created_at":"2026-05-18T01:20:34.578546+00:00"},{"alias_kind":"pith_short_12","alias_value":"V4JNSDQDY3ME","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"V4JNSDQDY3ME4P7V","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"V4JNSDQD","created_at":"2026-05-18T12:29:44.643036+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/V4JNSDQDY3ME4P7VPFKBLCZSAY","json":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY.json","graph_json":"https://pith.science/api/pith-number/V4JNSDQDY3ME4P7VPFKBLCZSAY/graph.json","events_json":"https://pith.science/api/pith-number/V4JNSDQDY3ME4P7VPFKBLCZSAY/events.json","paper":"https://pith.science/paper/V4JNSDQD"},"agent_actions":{"view_html":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY","download_json":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY.json","view_paper":"https://pith.science/paper/V4JNSDQD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1508.03413&json=true","fetch_graph":"https://pith.science/api/pith-number/V4JNSDQDY3ME4P7VPFKBLCZSAY/graph.json","fetch_events":"https://pith.science/api/pith-number/V4JNSDQDY3ME4P7VPFKBLCZSAY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY/action/storage_attestation","attest_author":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY/action/author_attestation","sign_citation":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY/action/citation_signature","submit_replication":"https://pith.science/pith/V4JNSDQDY3ME4P7VPFKBLCZSAY/action/replication_record"}},"created_at":"2026-05-18T01:20:34.578546+00:00","updated_at":"2026-05-18T01:20:34.578546+00:00"}