{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:PFK2MJ325HAFSB72W3JE6EBFER","short_pith_number":"pith:PFK2MJ32","canonical_record":{"source":{"id":"hep-th/9607156","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-07-18T12:42:12Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ee98db13f2dfed7046f07fd41507494343100c95d076332fca3411ca2236abec","abstract_canon_sha256":"0e795cb46e564792d502cc3551e29584ea59561fee59079db33f23e9f5d12c16"},"schema_version":"1.0"},"canonical_sha256":"7955a6277ae9c05907fab6d24f10252455046661f3e81ef5ef6e2c0ab2c9fbb6","source":{"kind":"arxiv","id":"hep-th/9607156","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9607156","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9607156v1","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9607156","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"pith_short_12","alias_value":"PFK2MJ325HAF","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PFK2MJ325HAFSB72","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PFK2MJ32","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:PFK2MJ325HAFSB72W3JE6EBFER","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9607156","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1996-07-18T12:42:12Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ee98db13f2dfed7046f07fd41507494343100c95d076332fca3411ca2236abec","abstract_canon_sha256":"0e795cb46e564792d502cc3551e29584ea59561fee59079db33f23e9f5d12c16"},"schema_version":"1.0"},"canonical_sha256":"7955a6277ae9c05907fab6d24f10252455046661f3e81ef5ef6e2c0ab2c9fbb6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:03.177766Z","signature_b64":"ilSZL3uC1KxPSl2aNLiBeu7giFjk94d35lXQCsFppbwBL8sH0ZeXO5kc6mKGvvrcG/SiGvslXdqCMWwF75bmDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7955a6277ae9c05907fab6d24f10252455046661f3e81ef5ef6e2c0ab2c9fbb6","last_reissued_at":"2026-05-18T02:36:03.177138Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:03.177138Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9607156","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":"2026-05-18T02:36:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aeTuG3NNYrxCNum3qFvdWNGnIwU8zwxNyTb613B7S7QkDbhVZjGw9Lv9DG5W7UigaKMTR+SRYMIFGEr51Z/7Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:06:59.158180Z"},"content_sha256":"9ee953c70c797557793f754a976fe1320c60dcb31e1a9a045ba08bfda2247a2f","schema_version":"1.0","event_id":"sha256:9ee953c70c797557793f754a976fe1320c60dcb31e1a9a045ba08bfda2247a2f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:PFK2MJ325HAFSB72W3JE6EBFER","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Perturbation Theory with a Variational Basis: the Generalized Gaussian Effective Potential","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Luigi Tedesco, Paolo Cea","submitted_at":"1996-07-18T12:42:12Z","abstract_excerpt":"The perturbation theory with a variational basis is constructed and analyzed.The generalized Gaussian effective potential is introduced and evaluated up to the second order for selfinteracting scalar fields in one and two spatial dimensions. The problem of the renormalization of the mass is discussed in details. Thermal corrections are incorporated. The comparison between the finite temperature generalized Gaussian effective potential and the finite temperature effective potential is critically analyzed. The phenomenon of the restoration at high temperature of the symmetry broken at zero tempe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9607156","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":"2026-05-18T02:36:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cq7SvZpmFfEbr+ZuE+2t9MMmTUJ8C/QPPNnsjYoliNDxgs69o0LX8vp1+czVzGy2EN0K4loTcT8ssBgmhxO/Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:06:59.158608Z"},"content_sha256":"5b37ea79ce44ed61d5f5402921153739bf5f0fb6947a13608291d56888113452","schema_version":"1.0","event_id":"sha256:5b37ea79ce44ed61d5f5402921153739bf5f0fb6947a13608291d56888113452"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PFK2MJ325HAFSB72W3JE6EBFER/bundle.json","state_url":"https://pith.science/pith/PFK2MJ325HAFSB72W3JE6EBFER/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PFK2MJ325HAFSB72W3JE6EBFER/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":"2026-05-30T13:06:59Z","links":{"resolver":"https://pith.science/pith/PFK2MJ325HAFSB72W3JE6EBFER","bundle":"https://pith.science/pith/PFK2MJ325HAFSB72W3JE6EBFER/bundle.json","state":"https://pith.science/pith/PFK2MJ325HAFSB72W3JE6EBFER/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PFK2MJ325HAFSB72W3JE6EBFER/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:PFK2MJ325HAFSB72W3JE6EBFER","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":"0e795cb46e564792d502cc3551e29584ea59561fee59079db33f23e9f5d12c16","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"1996-07-18T12:42:12Z","title_canon_sha256":"ee98db13f2dfed7046f07fd41507494343100c95d076332fca3411ca2236abec"},"schema_version":"1.0","source":{"id":"hep-th/9607156","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9607156","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9607156v1","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9607156","created_at":"2026-05-18T02:36:03Z"},{"alias_kind":"pith_short_12","alias_value":"PFK2MJ325HAF","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"PFK2MJ325HAFSB72","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"PFK2MJ32","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:5b37ea79ce44ed61d5f5402921153739bf5f0fb6947a13608291d56888113452","target":"graph","created_at":"2026-05-18T02:36:03Z","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":"The perturbation theory with a variational basis is constructed and analyzed.The generalized Gaussian effective potential is introduced and evaluated up to the second order for selfinteracting scalar fields in one and two spatial dimensions. The problem of the renormalization of the mass is discussed in details. Thermal corrections are incorporated. The comparison between the finite temperature generalized Gaussian effective potential and the finite temperature effective potential is critically analyzed. The phenomenon of the restoration at high temperature of the symmetry broken at zero tempe","authors_text":"Luigi Tedesco, Paolo Cea","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1996-07-18T12:42:12Z","title":"Perturbation Theory with a Variational Basis: the Generalized Gaussian Effective Potential"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9607156","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":"sha256:9ee953c70c797557793f754a976fe1320c60dcb31e1a9a045ba08bfda2247a2f","target":"record","created_at":"2026-05-18T02:36:03Z","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":"0e795cb46e564792d502cc3551e29584ea59561fee59079db33f23e9f5d12c16","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-th","submitted_at":"1996-07-18T12:42:12Z","title_canon_sha256":"ee98db13f2dfed7046f07fd41507494343100c95d076332fca3411ca2236abec"},"schema_version":"1.0","source":{"id":"hep-th/9607156","kind":"arxiv","version":1}},"canonical_sha256":"7955a6277ae9c05907fab6d24f10252455046661f3e81ef5ef6e2c0ab2c9fbb6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7955a6277ae9c05907fab6d24f10252455046661f3e81ef5ef6e2c0ab2c9fbb6","first_computed_at":"2026-05-18T02:36:03.177138Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:36:03.177138Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ilSZL3uC1KxPSl2aNLiBeu7giFjk94d35lXQCsFppbwBL8sH0ZeXO5kc6mKGvvrcG/SiGvslXdqCMWwF75bmDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:36:03.177766Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9607156","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9ee953c70c797557793f754a976fe1320c60dcb31e1a9a045ba08bfda2247a2f","sha256:5b37ea79ce44ed61d5f5402921153739bf5f0fb6947a13608291d56888113452"],"state_sha256":"374f1cbe4bd71a9bb0637af33c02da81064a96df6aa5162b1ef987cfc3567421"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ab8JMCHxsRDMEVAEx8ED7mg7rSwOxRTYHegYZ07F78yN8bjUzS/UdZDsHKbNgm5DTVe2sb1HBWXYnABfBxJKAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T13:06:59.161121Z","bundle_sha256":"bf3c7b172408fc25cedaea6482c1234f4680cf2902137274f5f18afbb435ed9a"}}