{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:DKMAWMFSL4IE4KLOHD56RPORTJ","short_pith_number":"pith:DKMAWMFS","canonical_record":{"source":{"id":"hep-ph/9801264","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-01-12T01:35:42Z","cross_cats_sorted":[],"title_canon_sha256":"a8720211deed98bccdb2fc21a5102cb7a5405c29ec21b29e96424110676a79fc","abstract_canon_sha256":"aa03769d16b442d573704426e6f78c19d28a37e02ff1a8c811666e701da92d87"},"schema_version":"1.0"},"canonical_sha256":"1a980b30b25f104e296e38fbe8bdd19a68344ff652932e4e1c5bfc8509548036","source":{"kind":"arxiv","id":"hep-ph/9801264","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9801264","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9801264v1","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9801264","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"DKMAWMFSL4IE","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"DKMAWMFSL4IE4KLO","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"DKMAWMFS","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:DKMAWMFSL4IE4KLOHD56RPORTJ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9801264","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-01-12T01:35:42Z","cross_cats_sorted":[],"title_canon_sha256":"a8720211deed98bccdb2fc21a5102cb7a5405c29ec21b29e96424110676a79fc","abstract_canon_sha256":"aa03769d16b442d573704426e6f78c19d28a37e02ff1a8c811666e701da92d87"},"schema_version":"1.0"},"canonical_sha256":"1a980b30b25f104e296e38fbe8bdd19a68344ff652932e4e1c5bfc8509548036","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:56.568519Z","signature_b64":"oZXt/HU7lz1ZHg319zIftRli/evkSz7MrnEJtmYBR87PDLSspKeN+Pd02+ch09gIyhxb1FrlxXsIDudg21bODw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a980b30b25f104e296e38fbe8bdd19a68344ff652932e4e1c5bfc8509548036","last_reissued_at":"2026-05-18T01:38:56.567992Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:56.567992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9801264","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":"2026-05-18T01:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CaqunhqAI+PDIrnxP1lINF9cJoghZmT2oeBPHa6stRGAmb3rCq0QRALBQxdekDCeY2WiatZ2GARDTiqZ76gaBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T18:33:00.359570Z"},"content_sha256":"1f52b04a3ef500b75a59d3def6966726af9f03531eaa092fa802c8431207e395","schema_version":"1.0","event_id":"sha256:1f52b04a3ef500b75a59d3def6966726af9f03531eaa092fa802c8431207e395"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:DKMAWMFSL4IE4KLOHD56RPORTJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"$\\lambda\\phi^4$ model and Higgs mass in standard model calculated by Gaussian effective potential approach with a new regularization-renormalization method","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fudan University, G.-j. Ni, J.-f Yang (Department of Physics, P. R. China), S.-y Lou, W.-f Lu","submitted_at":"1998-01-12T01:35:42Z","abstract_excerpt":"Basing on new regularization-renormalization method, the $\\lambda\\phi^4$ model used in standard model is studied both perturbatively and nonperturbatively (by Gaussian effective potential). The invariant property of two mass scales is stressed and the existence of a (Landau) pole is emphasized. Then after coupling with the SU(2)$\\times$U(1) gauge fields, the Higgs mass in standard model (SM) can be calculated as $m_H\\approx$138GeV. The critical temperature ($T_c$) for restoration of symmetry of Higgs field, the critical energy scale ($\\mu_c$, the maximum energy scale under which the lower exci"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9801264","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":"2026-05-18T01:38:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lGK8e23AvR3huWSXcBWVaFo9fjH7o5XC32/tlSzwf/m047DZpu9zKXjsX430N3i+ax2phYfpGvPdaGiOrqwUAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T18:33:00.360196Z"},"content_sha256":"4af89765c7eac07746afee32869605e460cd4e75ca354ee495a2f3c02fda4985","schema_version":"1.0","event_id":"sha256:4af89765c7eac07746afee32869605e460cd4e75ca354ee495a2f3c02fda4985"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/bundle.json","state_url":"https://pith.science/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/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":"2026-05-26T18:33:00Z","links":{"resolver":"https://pith.science/pith/DKMAWMFSL4IE4KLOHD56RPORTJ","bundle":"https://pith.science/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/bundle.json","state":"https://pith.science/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DKMAWMFSL4IE4KLOHD56RPORTJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:DKMAWMFSL4IE4KLOHD56RPORTJ","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":"aa03769d16b442d573704426e6f78c19d28a37e02ff1a8c811666e701da92d87","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-01-12T01:35:42Z","title_canon_sha256":"a8720211deed98bccdb2fc21a5102cb7a5405c29ec21b29e96424110676a79fc"},"schema_version":"1.0","source":{"id":"hep-ph/9801264","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9801264","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9801264v1","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9801264","created_at":"2026-05-18T01:38:56Z"},{"alias_kind":"pith_short_12","alias_value":"DKMAWMFSL4IE","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"DKMAWMFSL4IE4KLO","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"DKMAWMFS","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:4af89765c7eac07746afee32869605e460cd4e75ca354ee495a2f3c02fda4985","target":"graph","created_at":"2026-05-18T01:38:56Z","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":"Basing on new regularization-renormalization method, the $\\lambda\\phi^4$ model used in standard model is studied both perturbatively and nonperturbatively (by Gaussian effective potential). The invariant property of two mass scales is stressed and the existence of a (Landau) pole is emphasized. Then after coupling with the SU(2)$\\times$U(1) gauge fields, the Higgs mass in standard model (SM) can be calculated as $m_H\\approx$138GeV. The critical temperature ($T_c$) for restoration of symmetry of Higgs field, the critical energy scale ($\\mu_c$, the maximum energy scale under which the lower exci","authors_text":"Fudan University, G.-j. Ni, J.-f Yang (Department of Physics, P. R. China), S.-y Lou, W.-f Lu","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-01-12T01:35:42Z","title":"$\\lambda\\phi^4$ model and Higgs mass in standard model calculated by Gaussian effective potential approach with a new regularization-renormalization method"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9801264","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":"sha256:1f52b04a3ef500b75a59d3def6966726af9f03531eaa092fa802c8431207e395","target":"record","created_at":"2026-05-18T01:38:56Z","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":"aa03769d16b442d573704426e6f78c19d28a37e02ff1a8c811666e701da92d87","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1998-01-12T01:35:42Z","title_canon_sha256":"a8720211deed98bccdb2fc21a5102cb7a5405c29ec21b29e96424110676a79fc"},"schema_version":"1.0","source":{"id":"hep-ph/9801264","kind":"arxiv","version":1}},"canonical_sha256":"1a980b30b25f104e296e38fbe8bdd19a68344ff652932e4e1c5bfc8509548036","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1a980b30b25f104e296e38fbe8bdd19a68344ff652932e4e1c5bfc8509548036","first_computed_at":"2026-05-18T01:38:56.567992Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:56.567992Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oZXt/HU7lz1ZHg319zIftRli/evkSz7MrnEJtmYBR87PDLSspKeN+Pd02+ch09gIyhxb1FrlxXsIDudg21bODw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:56.568519Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9801264","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1f52b04a3ef500b75a59d3def6966726af9f03531eaa092fa802c8431207e395","sha256:4af89765c7eac07746afee32869605e460cd4e75ca354ee495a2f3c02fda4985"],"state_sha256":"d17b45374924a3cbf4286f2a17ff6ff3ed41facc1a6597d5d05236fe95853159"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wP8C3vRpVPZLLJ7rNIpZPHK5Oq9gOKXsqSh49QnlzGm0ywLpeA3LMCTZOjw48xRVz02wm+1tV2ZJWGYXlTU9Cg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T18:33:00.363270Z","bundle_sha256":"87de707bf2ea8d0b8525f162fca8a0311891ebcab6fff4c26c2b3e195fdf820c"}}