{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:PEYLGDUW5LPQNRBNGXAVNO3GJO","short_pith_number":"pith:PEYLGDUW","canonical_record":{"source":{"id":"hep-ph/0210388","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-10-28T19:48:18Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"3575bc95c62a536e958f7c4c896b6823b46b8037b1e3b8ed6ed3a14012f06925","abstract_canon_sha256":"afe46c3e8a8a29f939a080a59d9ecccc340e78a24449db2e9e90a21cbc384b90"},"schema_version":"1.0"},"canonical_sha256":"7930b30e96eadf06c42d35c156bb664bbad864fcf07ed2100caae5dffd7ca34f","source":{"kind":"arxiv","id":"hep-ph/0210388","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0210388","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0210388v3","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0210388","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_12","alias_value":"PEYLGDUW5LPQ","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_16","alias_value":"PEYLGDUW5LPQNRBN","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_8","alias_value":"PEYLGDUW","created_at":"2026-07-04T16:34:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:PEYLGDUW5LPQNRBNGXAVNO3GJO","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0210388","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-10-28T19:48:18Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"3575bc95c62a536e958f7c4c896b6823b46b8037b1e3b8ed6ed3a14012f06925","abstract_canon_sha256":"afe46c3e8a8a29f939a080a59d9ecccc340e78a24449db2e9e90a21cbc384b90"},"schema_version":"1.0"},"canonical_sha256":"7930b30e96eadf06c42d35c156bb664bbad864fcf07ed2100caae5dffd7ca34f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:24.807299Z","signature_b64":"aVNSS3vGr62AG2ENYH4ts2xjpKtMWAoiTxBZkywRokFvOb5XvAyxBb93Hc2U11TBARwnKyyu1nlyWudfBdhuBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7930b30e96eadf06c42d35c156bb664bbad864fcf07ed2100caae5dffd7ca34f","last_reissued_at":"2026-07-04T16:34:24.806955Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:24.806955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0210388","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:34:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KuzSLTzrxU9puQ4tC1vXrIvpP+ZGSW7SkaUAQ9uBhPgatD6WbL0hqJ2ADmeBfYOEqO8Xgu4JcPF6NLhOLWGoBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T04:15:43.527807Z"},"content_sha256":"292ec91d0eb3d9db8f6c616b24e1a694fe3a08a17945642273534a9e0a23ca3c","schema_version":"1.0","event_id":"sha256:292ec91d0eb3d9db8f6c616b24e1a694fe3a08a17945642273534a9e0a23ca3c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:PEYLGDUW5LPQNRBNGXAVNO3GJO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalization Group and Decoupling in Curved Space","license":"","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"E.V. Gorbar, I.L. Shapiro","submitted_at":"2002-10-28T19:48:18Z","abstract_excerpt":"It is well known that the renormalization group equations depend on the scale where they are applied. This phenomenon is especially relevant for the massive fields in curved space, because the decoupling effects may be responsible for important cosmological applications like the graceful exit from the inflation and low-energy quantum dynamics of the cosmological constant. We investigate, using both covariant and non-covariant methods of calculations and mass-dependent renormalization scheme, the vacuum quantum effects of a massive scalar field in curved space-time. In the higher derivative sec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0210388","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-ph/0210388/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:34:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gMBQloDSaH7oPiSNhgKMAxiGrjIqxVrIH5Wivy6e4xE45flfdw3ccBoPEAmDwmgGQyFHng4u9rP6C8L5xdMCAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T04:15:43.528600Z"},"content_sha256":"90a971530ca4332e409a1f8ecef1ebce451b55de7cbe06c18c18529dfe2c640a","schema_version":"1.0","event_id":"sha256:90a971530ca4332e409a1f8ecef1ebce451b55de7cbe06c18c18529dfe2c640a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/bundle.json","state_url":"https://pith.science/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-04T04:15:43Z","links":{"resolver":"https://pith.science/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO","bundle":"https://pith.science/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/bundle.json","state":"https://pith.science/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PEYLGDUW5LPQNRBNGXAVNO3GJO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:PEYLGDUW5LPQNRBNGXAVNO3GJO","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"afe46c3e8a8a29f939a080a59d9ecccc340e78a24449db2e9e90a21cbc384b90","cross_cats_sorted":["gr-qc","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-10-28T19:48:18Z","title_canon_sha256":"3575bc95c62a536e958f7c4c896b6823b46b8037b1e3b8ed6ed3a14012f06925"},"schema_version":"1.0","source":{"id":"hep-ph/0210388","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0210388","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0210388v3","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0210388","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_12","alias_value":"PEYLGDUW5LPQ","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_16","alias_value":"PEYLGDUW5LPQNRBN","created_at":"2026-07-04T16:34:24Z"},{"alias_kind":"pith_short_8","alias_value":"PEYLGDUW","created_at":"2026-07-04T16:34:24Z"}],"graph_snapshots":[{"event_id":"sha256:90a971530ca4332e409a1f8ecef1ebce451b55de7cbe06c18c18529dfe2c640a","target":"graph","created_at":"2026-07-04T16:34:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/0210388/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It is well known that the renormalization group equations depend on the scale where they are applied. This phenomenon is especially relevant for the massive fields in curved space, because the decoupling effects may be responsible for important cosmological applications like the graceful exit from the inflation and low-energy quantum dynamics of the cosmological constant. We investigate, using both covariant and non-covariant methods of calculations and mass-dependent renormalization scheme, the vacuum quantum effects of a massive scalar field in curved space-time. In the higher derivative sec","authors_text":"E.V. Gorbar, I.L. Shapiro","cross_cats":["gr-qc","hep-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2002-10-28T19:48:18Z","title":"Renormalization Group and Decoupling in Curved Space"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0210388","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:292ec91d0eb3d9db8f6c616b24e1a694fe3a08a17945642273534a9e0a23ca3c","target":"record","created_at":"2026-07-04T16:34:24Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"afe46c3e8a8a29f939a080a59d9ecccc340e78a24449db2e9e90a21cbc384b90","cross_cats_sorted":["gr-qc","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-10-28T19:48:18Z","title_canon_sha256":"3575bc95c62a536e958f7c4c896b6823b46b8037b1e3b8ed6ed3a14012f06925"},"schema_version":"1.0","source":{"id":"hep-ph/0210388","kind":"arxiv","version":3}},"canonical_sha256":"7930b30e96eadf06c42d35c156bb664bbad864fcf07ed2100caae5dffd7ca34f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7930b30e96eadf06c42d35c156bb664bbad864fcf07ed2100caae5dffd7ca34f","first_computed_at":"2026-07-04T16:34:24.806955Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:34:24.806955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aVNSS3vGr62AG2ENYH4ts2xjpKtMWAoiTxBZkywRokFvOb5XvAyxBb93Hc2U11TBARwnKyyu1nlyWudfBdhuBg==","signature_status":"signed_v1","signed_at":"2026-07-04T16:34:24.807299Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0210388","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:292ec91d0eb3d9db8f6c616b24e1a694fe3a08a17945642273534a9e0a23ca3c","sha256:90a971530ca4332e409a1f8ecef1ebce451b55de7cbe06c18c18529dfe2c640a"],"state_sha256":"2c1d18e36b6d2769a32635ca681c469f499b121fe3fe6fe5e51fbbe8dadd1530"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lC4ouyn29Bqy6rxmLHEc5m9JfwflsJXk/xp0kTw2DIUe/sSGXvLCfWQj/2xw5GUOf8lkWj1qPv3CuHBEHALBAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T04:15:43.534910Z","bundle_sha256":"af3046d1f5acf6fd93d315bc72c057346bd63ff8c72c342395cdedae037d84df"}}