{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:KD2M4A2YIRZMI6NZNACMDZX32Q","short_pith_number":"pith:KD2M4A2Y","canonical_record":{"source":{"id":"1210.1163","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-10-03T16:14:23Z","cross_cats_sorted":[],"title_canon_sha256":"cf2415898fedcff7ed8fe996402015baee1284aff4341b4da40d2ae8e0f5350b","abstract_canon_sha256":"79e1d991cb4ce2b73846ef47d1efb787b21115f99bfa4fc4631b70042c65d0fe"},"schema_version":"1.0"},"canonical_sha256":"50f4ce03584472c479b96804c1e6fbd411c70759133c72555d25084a286cf6b0","source":{"kind":"arxiv","id":"1210.1163","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.1163","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"arxiv_version","alias_value":"1210.1163v1","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.1163","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"pith_short_12","alias_value":"KD2M4A2YIRZM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KD2M4A2YIRZMI6NZ","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KD2M4A2Y","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:KD2M4A2YIRZMI6NZNACMDZX32Q","target":"record","payload":{"canonical_record":{"source":{"id":"1210.1163","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-10-03T16:14:23Z","cross_cats_sorted":[],"title_canon_sha256":"cf2415898fedcff7ed8fe996402015baee1284aff4341b4da40d2ae8e0f5350b","abstract_canon_sha256":"79e1d991cb4ce2b73846ef47d1efb787b21115f99bfa4fc4631b70042c65d0fe"},"schema_version":"1.0"},"canonical_sha256":"50f4ce03584472c479b96804c1e6fbd411c70759133c72555d25084a286cf6b0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:44:05.352132Z","signature_b64":"x3TLGMLmU6qnJPw75nEz46L+j03rxUf/QlbYQjV4jLtr8J6wBpIphyTJSBUXZ5dASwkJcIa43tEDZ2gw+KhdBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50f4ce03584472c479b96804c1e6fbd411c70759133c72555d25084a286cf6b0","last_reissued_at":"2026-05-18T03:44:05.351414Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:44:05.351414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.1163","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:44:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zl5TzL5x268qo3Lt0qIqNbWdRI11UKoQUVhHjJcEPT1r8Gb7TSdbmIX9d8PIhEH2V67F/K+Q5Wyp+o2+iGqRAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:53:24.033408Z"},"content_sha256":"d3156db8549f36a80c61c0f004a39db750ac8f625865370cce7c6aa514548021","schema_version":"1.0","event_id":"sha256:d3156db8549f36a80c61c0f004a39db750ac8f625865370cce7c6aa514548021"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:KD2M4A2YIRZMI6NZNACMDZX32Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vilkovisky-DeWitt Effective Potential Revisited in Gauge-Free Framework","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Srijit Bhattacharjee","submitted_at":"2012-10-03T16:14:23Z","abstract_excerpt":"An alternative approach to scalar quantum electrodynamics has been proposed where the usual gauge redundancy of the theory do not manifest. The gauge-dependence of Coleman- Weinberg effective potential is resolved using gauge-free approach leading to a unique scalar to vector mass ratio. The gauge-free result is compared with the one obtained in Vilkovisky-DeWitt geometric framework and it is shown that it differs from the standard result reported earlier. It is also shown that for reparametrization invariance of the Coleman-Weinberg potential one must combine the Vilkovisky-DeWitt method with"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.1163","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:44:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tSWYQLMi/WoQEgjeXttDmGkK++kBgXI8BQdWnjzYRkvf0A+ASo9khDQDTjCkROw8FPOiLADP+1eUw/Jtlqz6AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T01:53:24.033768Z"},"content_sha256":"b8fbc6cdce389b96820ed2346af76e62bd0d83ffa726199bbfad957b916d2cd8","schema_version":"1.0","event_id":"sha256:b8fbc6cdce389b96820ed2346af76e62bd0d83ffa726199bbfad957b916d2cd8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/bundle.json","state_url":"https://pith.science/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/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":"2026-05-27T01:53:24Z","links":{"resolver":"https://pith.science/pith/KD2M4A2YIRZMI6NZNACMDZX32Q","bundle":"https://pith.science/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/bundle.json","state":"https://pith.science/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KD2M4A2YIRZMI6NZNACMDZX32Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:KD2M4A2YIRZMI6NZNACMDZX32Q","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":"79e1d991cb4ce2b73846ef47d1efb787b21115f99bfa4fc4631b70042c65d0fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-10-03T16:14:23Z","title_canon_sha256":"cf2415898fedcff7ed8fe996402015baee1284aff4341b4da40d2ae8e0f5350b"},"schema_version":"1.0","source":{"id":"1210.1163","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.1163","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"arxiv_version","alias_value":"1210.1163v1","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.1163","created_at":"2026-05-18T03:44:05Z"},{"alias_kind":"pith_short_12","alias_value":"KD2M4A2YIRZM","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KD2M4A2YIRZMI6NZ","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KD2M4A2Y","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:b8fbc6cdce389b96820ed2346af76e62bd0d83ffa726199bbfad957b916d2cd8","target":"graph","created_at":"2026-05-18T03:44:05Z","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"},"paper":{"abstract_excerpt":"An alternative approach to scalar quantum electrodynamics has been proposed where the usual gauge redundancy of the theory do not manifest. The gauge-dependence of Coleman- Weinberg effective potential is resolved using gauge-free approach leading to a unique scalar to vector mass ratio. The gauge-free result is compared with the one obtained in Vilkovisky-DeWitt geometric framework and it is shown that it differs from the standard result reported earlier. It is also shown that for reparametrization invariance of the Coleman-Weinberg potential one must combine the Vilkovisky-DeWitt method with","authors_text":"Srijit Bhattacharjee","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-10-03T16:14:23Z","title":"Vilkovisky-DeWitt Effective Potential Revisited in Gauge-Free Framework"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.1163","kind":"arxiv","version":1},"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:d3156db8549f36a80c61c0f004a39db750ac8f625865370cce7c6aa514548021","target":"record","created_at":"2026-05-18T03:44:05Z","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":"79e1d991cb4ce2b73846ef47d1efb787b21115f99bfa4fc4631b70042c65d0fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-10-03T16:14:23Z","title_canon_sha256":"cf2415898fedcff7ed8fe996402015baee1284aff4341b4da40d2ae8e0f5350b"},"schema_version":"1.0","source":{"id":"1210.1163","kind":"arxiv","version":1}},"canonical_sha256":"50f4ce03584472c479b96804c1e6fbd411c70759133c72555d25084a286cf6b0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"50f4ce03584472c479b96804c1e6fbd411c70759133c72555d25084a286cf6b0","first_computed_at":"2026-05-18T03:44:05.351414Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:44:05.351414Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"x3TLGMLmU6qnJPw75nEz46L+j03rxUf/QlbYQjV4jLtr8J6wBpIphyTJSBUXZ5dASwkJcIa43tEDZ2gw+KhdBw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:44:05.352132Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.1163","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d3156db8549f36a80c61c0f004a39db750ac8f625865370cce7c6aa514548021","sha256:b8fbc6cdce389b96820ed2346af76e62bd0d83ffa726199bbfad957b916d2cd8"],"state_sha256":"2513d2d4aad001531ac5e38dbbf80211f7e2bc7f6d5714eacabd8a6b842f1441"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g7gOvdpOe517Q8tkRCDjga21xhmMg2/gX2GJ9ve1GrSXTxldIauWN6g8VCJcquk/9x5NIDpdRfl9pYgCc1hNDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T01:53:24.036178Z","bundle_sha256":"d4b40007be56091349d6fb9a21c3ee3693f106826674ab7bbe6d97a03270d5c0"}}