{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:JUUJEN2IQFCGUJIXPQFWTQMLEK","short_pith_number":"pith:JUUJEN2I","canonical_record":{"source":{"id":"1509.01466","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-04T14:33:23Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bccb7bf7b34c0056fc4866a732af9c4bb6a67fd5d760a6558ef78947e08be160","abstract_canon_sha256":"1e3f1d94b518d4a579cea3839863c5f77fb5b04a1fb009c6ba522aebac962742"},"schema_version":"1.0"},"canonical_sha256":"4d2892374881446a25177c0b69c18b22b64dfdbe9efec44e580c5e1643f096b6","source":{"kind":"arxiv","id":"1509.01466","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.01466","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"arxiv_version","alias_value":"1509.01466v4","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.01466","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"pith_short_12","alias_value":"JUUJEN2IQFCG","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"JUUJEN2IQFCGUJIX","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"JUUJEN2I","created_at":"2026-05-18T12:29:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:JUUJEN2IQFCGUJIXPQFWTQMLEK","target":"record","payload":{"canonical_record":{"source":{"id":"1509.01466","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-04T14:33:23Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bccb7bf7b34c0056fc4866a732af9c4bb6a67fd5d760a6558ef78947e08be160","abstract_canon_sha256":"1e3f1d94b518d4a579cea3839863c5f77fb5b04a1fb009c6ba522aebac962742"},"schema_version":"1.0"},"canonical_sha256":"4d2892374881446a25177c0b69c18b22b64dfdbe9efec44e580c5e1643f096b6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:57.724427Z","signature_b64":"q+gpCpGNDIgze/vXGlDdT79ZHIzBf5lljo56d6GKA7tQ5wqdn/IieCLLZFNlREhmsWIOoT1Q3OUVmxXJYVTzAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4d2892374881446a25177c0b69c18b22b64dfdbe9efec44e580c5e1643f096b6","last_reissued_at":"2026-05-18T00:50:57.723875Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:57.723875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.01466","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:50:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FKWa4yUvYRtDwe1ISQRzMWGTaAR7Y6E2thEvwxEaHXoLDO7dFx0JMX2a1bxMvLLpszRNx/MtuT59nGGy8ftNAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T17:24:46.312140Z"},"content_sha256":"58691272fb1be948c0abceaff9ed665900395587214bc1aa53961cd9bb0dccf9","schema_version":"1.0","event_id":"sha256:58691272fb1be948c0abceaff9ed665900395587214bc1aa53961cd9bb0dccf9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:JUUJEN2IQFCGUJIXPQFWTQMLEK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Electroweak vacuum stability in classically conformal B-L extension of the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Arindam Das, Nathan Papapietro, Nobuchika Okada","submitted_at":"2015-09-04T14:33:23Z","abstract_excerpt":"We consider the minimal U(1)$_{B-L}$ extension of the Standard Model (SM) with the classically conformal invariance, where an anomaly free U(1)$_{B-L}$ gauge symmetry is introduced along with three generations of right-handed neutrinos and a U(1)$_{B-L}$ Higgs field. Because of the classically conformal symmetry, all dimensional parameters are forbidden. The $B-L$ gauge symmetry is radiatively broken through the Coleman-Weinberg mechanism, generating the mass for the $U(1)_{B-L}$ gauge boson ($Z^\\prime$ boson) and the right-handed neutrinos. Through a small negative coupling between the SM Hig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.01466","kind":"arxiv","version":4},"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":"2026-05-18T00:50:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BiR6V5zvNlf2SF4+S48c1MQkZBuv8Wqgvas9D7taumIDYw8k+IZ8HhlMkIlq24J1c/FO+HNvj6+Th88AmmptCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T17:24:46.312530Z"},"content_sha256":"23e1fe6a50deb64cdac7d769a33fc7e2ba27d3fde0cec21c83efd125657c4867","schema_version":"1.0","event_id":"sha256:23e1fe6a50deb64cdac7d769a33fc7e2ba27d3fde0cec21c83efd125657c4867"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/bundle.json","state_url":"https://pith.science/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/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":"2026-05-21T17:24:46Z","links":{"resolver":"https://pith.science/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK","bundle":"https://pith.science/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/bundle.json","state":"https://pith.science/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JUUJEN2IQFCGUJIXPQFWTQMLEK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:JUUJEN2IQFCGUJIXPQFWTQMLEK","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":"1e3f1d94b518d4a579cea3839863c5f77fb5b04a1fb009c6ba522aebac962742","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-04T14:33:23Z","title_canon_sha256":"bccb7bf7b34c0056fc4866a732af9c4bb6a67fd5d760a6558ef78947e08be160"},"schema_version":"1.0","source":{"id":"1509.01466","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.01466","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"arxiv_version","alias_value":"1509.01466v4","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.01466","created_at":"2026-05-18T00:50:57Z"},{"alias_kind":"pith_short_12","alias_value":"JUUJEN2IQFCG","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_16","alias_value":"JUUJEN2IQFCGUJIX","created_at":"2026-05-18T12:29:27Z"},{"alias_kind":"pith_short_8","alias_value":"JUUJEN2I","created_at":"2026-05-18T12:29:27Z"}],"graph_snapshots":[{"event_id":"sha256:23e1fe6a50deb64cdac7d769a33fc7e2ba27d3fde0cec21c83efd125657c4867","target":"graph","created_at":"2026-05-18T00:50:57Z","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":"We consider the minimal U(1)$_{B-L}$ extension of the Standard Model (SM) with the classically conformal invariance, where an anomaly free U(1)$_{B-L}$ gauge symmetry is introduced along with three generations of right-handed neutrinos and a U(1)$_{B-L}$ Higgs field. Because of the classically conformal symmetry, all dimensional parameters are forbidden. The $B-L$ gauge symmetry is radiatively broken through the Coleman-Weinberg mechanism, generating the mass for the $U(1)_{B-L}$ gauge boson ($Z^\\prime$ boson) and the right-handed neutrinos. Through a small negative coupling between the SM Hig","authors_text":"Arindam Das, Nathan Papapietro, Nobuchika Okada","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-04T14:33:23Z","title":"Electroweak vacuum stability in classically conformal B-L extension of the Standard Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.01466","kind":"arxiv","version":4},"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":"sha256:58691272fb1be948c0abceaff9ed665900395587214bc1aa53961cd9bb0dccf9","target":"record","created_at":"2026-05-18T00:50:57Z","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":"1e3f1d94b518d4a579cea3839863c5f77fb5b04a1fb009c6ba522aebac962742","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-04T14:33:23Z","title_canon_sha256":"bccb7bf7b34c0056fc4866a732af9c4bb6a67fd5d760a6558ef78947e08be160"},"schema_version":"1.0","source":{"id":"1509.01466","kind":"arxiv","version":4}},"canonical_sha256":"4d2892374881446a25177c0b69c18b22b64dfdbe9efec44e580c5e1643f096b6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4d2892374881446a25177c0b69c18b22b64dfdbe9efec44e580c5e1643f096b6","first_computed_at":"2026-05-18T00:50:57.723875Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:50:57.723875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"q+gpCpGNDIgze/vXGlDdT79ZHIzBf5lljo56d6GKA7tQ5wqdn/IieCLLZFNlREhmsWIOoT1Q3OUVmxXJYVTzAg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:50:57.724427Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.01466","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:58691272fb1be948c0abceaff9ed665900395587214bc1aa53961cd9bb0dccf9","sha256:23e1fe6a50deb64cdac7d769a33fc7e2ba27d3fde0cec21c83efd125657c4867"],"state_sha256":"e140ae068168e24d43645e29ef6a523e2d67d2a675505b24492ab2408ed33d0d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LRgs4utgt6LIK3zZRoO6bPkTjAZOubLY3qt0kVunIbIOe3F3UATF7qHVIHZMGDNhjHUWnHwPuKOL0OtwD6q1Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T17:24:46.315163Z","bundle_sha256":"3ba05e34811a94d151554d84af6756633beed64bcf274406850f18ae3a511ec4"}}