{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:2LWAO4QFOOG4O7F34L5NPHJIAA","short_pith_number":"pith:2LWAO4QF","canonical_record":{"source":{"id":"1803.03902","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-11T04:38:52Z","cross_cats_sorted":[],"title_canon_sha256":"5b06cb722106a3ddcbf1f567051efb1a670f20dc4e37d0aa2b4bc2c1055e876d","abstract_canon_sha256":"627d98607556d15c455329a76309ceccc9706bac30b2102b4b5fe1ea1c1a825b"},"schema_version":"1.0"},"canonical_sha256":"d2ec077205738dc77cbbe2fad79d28002753ee8e38d672050db961c3f7fda029","source":{"kind":"arxiv","id":"1803.03902","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.03902","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"arxiv_version","alias_value":"1803.03902v2","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.03902","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"pith_short_12","alias_value":"2LWAO4QFOOG4","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"2LWAO4QFOOG4O7F3","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"2LWAO4QF","created_at":"2026-05-18T12:32:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:2LWAO4QFOOG4O7F34L5NPHJIAA","target":"record","payload":{"canonical_record":{"source":{"id":"1803.03902","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-11T04:38:52Z","cross_cats_sorted":[],"title_canon_sha256":"5b06cb722106a3ddcbf1f567051efb1a670f20dc4e37d0aa2b4bc2c1055e876d","abstract_canon_sha256":"627d98607556d15c455329a76309ceccc9706bac30b2102b4b5fe1ea1c1a825b"},"schema_version":"1.0"},"canonical_sha256":"d2ec077205738dc77cbbe2fad79d28002753ee8e38d672050db961c3f7fda029","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:52.852259Z","signature_b64":"flZpZV2YD6gFl+OpZprF5W0C2dfWWwcFIj1jyMpF+kFmiRp57e9UYaK/5cuubiQkCBw21J4txJvsPbFNRM0ZBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2ec077205738dc77cbbe2fad79d28002753ee8e38d672050db961c3f7fda029","last_reissued_at":"2026-05-18T00:12:52.851769Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:52.851769Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1803.03902","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:12:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7nAG/jwYgJDaw0YO9/XjQqiyPRnJIqcjgLq+4m/MEtm0vZcaVnuxzAixuQwp6gs1Yi5/a1YbrPnoWzQsB0AOAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T10:50:36.508282Z"},"content_sha256":"8fde82c8b9997946c307e6180e5e77fac67a3bb82f542ad1e6466fcb9e1dd936","schema_version":"1.0","event_id":"sha256:8fde82c8b9997946c307e6180e5e77fac67a3bb82f542ad1e6466fcb9e1dd936"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:2LWAO4QFOOG4O7F34L5NPHJIAA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Decay Rate of Electroweak Vacuum in the Standard Model and Beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"So Chigusa, Takeo Moroi, Yutaro Shoji","submitted_at":"2018-03-11T04:38:52Z","abstract_excerpt":"We perform a precise calculation of the decay rate of the electroweak vacuum in the standard model as well as in models beyond the standard model. We use a recently-developed technique to calculate the decay rate of a false vacuum, which provides a gauge invariant calculation of the decay rate at the one-loop level. We give a prescription to take into account the zero modes in association with translational, dilatational, and gauge symmetries. We calculate the decay rate per unit volume, $\\gamma$, by using an analytic formula. The decay rate of the electroweak vacuum in the standard model is e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.03902","kind":"arxiv","version":2},"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":"2026-05-18T00:12:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"44o0gYzlH3DJuTQLR/BwtBda1ETf0UE4SMXRPlVN2vGxhqkra9LUY2neLJYA2V693nny7za0FRa9HxdbEoMlBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T10:50:36.508646Z"},"content_sha256":"3edeb5f45eb99143c3df0238aaad48a447ecf03f9d68494812006b6a0f29fe44","schema_version":"1.0","event_id":"sha256:3edeb5f45eb99143c3df0238aaad48a447ecf03f9d68494812006b6a0f29fe44"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/bundle.json","state_url":"https://pith.science/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/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":"2026-06-09T10:50:36Z","links":{"resolver":"https://pith.science/pith/2LWAO4QFOOG4O7F34L5NPHJIAA","bundle":"https://pith.science/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/bundle.json","state":"https://pith.science/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2LWAO4QFOOG4O7F34L5NPHJIAA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:2LWAO4QFOOG4O7F34L5NPHJIAA","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":"627d98607556d15c455329a76309ceccc9706bac30b2102b4b5fe1ea1c1a825b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-11T04:38:52Z","title_canon_sha256":"5b06cb722106a3ddcbf1f567051efb1a670f20dc4e37d0aa2b4bc2c1055e876d"},"schema_version":"1.0","source":{"id":"1803.03902","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1803.03902","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"arxiv_version","alias_value":"1803.03902v2","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.03902","created_at":"2026-05-18T00:12:52Z"},{"alias_kind":"pith_short_12","alias_value":"2LWAO4QFOOG4","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"2LWAO4QFOOG4O7F3","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"2LWAO4QF","created_at":"2026-05-18T12:32:02Z"}],"graph_snapshots":[{"event_id":"sha256:3edeb5f45eb99143c3df0238aaad48a447ecf03f9d68494812006b6a0f29fe44","target":"graph","created_at":"2026-05-18T00:12:52Z","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 perform a precise calculation of the decay rate of the electroweak vacuum in the standard model as well as in models beyond the standard model. We use a recently-developed technique to calculate the decay rate of a false vacuum, which provides a gauge invariant calculation of the decay rate at the one-loop level. We give a prescription to take into account the zero modes in association with translational, dilatational, and gauge symmetries. We calculate the decay rate per unit volume, $\\gamma$, by using an analytic formula. The decay rate of the electroweak vacuum in the standard model is e","authors_text":"So Chigusa, Takeo Moroi, Yutaro Shoji","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-11T04:38:52Z","title":"Decay Rate of Electroweak Vacuum in the Standard Model and Beyond"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.03902","kind":"arxiv","version":2},"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":"sha256:8fde82c8b9997946c307e6180e5e77fac67a3bb82f542ad1e6466fcb9e1dd936","target":"record","created_at":"2026-05-18T00:12:52Z","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":"627d98607556d15c455329a76309ceccc9706bac30b2102b4b5fe1ea1c1a825b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-03-11T04:38:52Z","title_canon_sha256":"5b06cb722106a3ddcbf1f567051efb1a670f20dc4e37d0aa2b4bc2c1055e876d"},"schema_version":"1.0","source":{"id":"1803.03902","kind":"arxiv","version":2}},"canonical_sha256":"d2ec077205738dc77cbbe2fad79d28002753ee8e38d672050db961c3f7fda029","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d2ec077205738dc77cbbe2fad79d28002753ee8e38d672050db961c3f7fda029","first_computed_at":"2026-05-18T00:12:52.851769Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:12:52.851769Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"flZpZV2YD6gFl+OpZprF5W0C2dfWWwcFIj1jyMpF+kFmiRp57e9UYaK/5cuubiQkCBw21J4txJvsPbFNRM0ZBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:12:52.852259Z","signed_message":"canonical_sha256_bytes"},"source_id":"1803.03902","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8fde82c8b9997946c307e6180e5e77fac67a3bb82f542ad1e6466fcb9e1dd936","sha256:3edeb5f45eb99143c3df0238aaad48a447ecf03f9d68494812006b6a0f29fe44"],"state_sha256":"392921c23e787f7611b72b96a68a856e4cd042fd2c4c123d2994234a8f37733b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"anWpnB3mjrSxhfBeqSbNYVIr1241AGiLqUOjZGM5Tr7490aYARQlAPB5Paxu5Cf/HCq9B2Y48tSLUB7W10o5Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T10:50:36.510469Z","bundle_sha256":"b1555404d462193f50c923957baf6e659b2e07d645cbca484a89a7fe6ae4c46e"}}