{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:CAIBUP4P2N7LE3C5RAFRHQID2W","short_pith_number":"pith:CAIBUP4P","canonical_record":{"source":{"id":"1404.7450","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-29T18:21:12Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"8ed17630fe224dfe866f513537bd0417b1867bf9f82733e400dc40ad9254417f","abstract_canon_sha256":"f6c87a59bb920b26a1a6defc2a924572a66edb9fa69dd0e432fa7fcd86dafbe1"},"schema_version":"1.0"},"canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","source":{"kind":"arxiv","id":"1404.7450","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.7450","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"1404.7450v2","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7450","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"CAIBUP4P2N7L","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CAIBUP4P2N7LE3C5","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CAIBUP4P","created_at":"2026-05-18T12:28:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:CAIBUP4P2N7LE3C5RAFRHQID2W","target":"record","payload":{"canonical_record":{"source":{"id":"1404.7450","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-29T18:21:12Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"8ed17630fe224dfe866f513537bd0417b1867bf9f82733e400dc40ad9254417f","abstract_canon_sha256":"f6c87a59bb920b26a1a6defc2a924572a66edb9fa69dd0e432fa7fcd86dafbe1"},"schema_version":"1.0"},"canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:43:21.849809Z","signature_b64":"BcBdHWS6yHUHMAs0yVJgZCvdYXC66Iu4WQPBO6WEBu0N7X5OkyAXw9OaHU33HZQitOH+r/g3cmMvmERwuVTOBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","last_reissued_at":"2026-05-18T01:43:21.849181Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:43:21.849181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.7450","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":"2026-05-18T01:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"f0iTqZ+qlY02B8r+hrmoz2ilZRK+j6LqNOdvnYNVP0uJTCXWnHD0h3J9BYs77PO5hfIeTALMGNatGlCmxaObAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T10:24:37.611171Z"},"content_sha256":"fdd4c20ae0b015b190434af5601913d718202c7933e8fe4cc0105ad3a7964ee2","schema_version":"1.0","event_id":"sha256:fdd4c20ae0b015b190434af5601913d718202c7933e8fe4cc0105ad3a7964ee2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:CAIBUP4P2N7LE3C5RAFRHQID2W","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the gauge dependence of the Standard Model vacuum instability scale","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Luca Di Luzio, Luminita Mihaila","submitted_at":"2014-04-29T18:21:12Z","abstract_excerpt":"After reviewing the calculation of the Standard Model one-loop effective potential in a class of linear gauges, we discuss the physical observables entering the vacuum stability analysis. While the electroweak-vacuum-stability bound on the Higgs boson mass can be formally proven to be gauge independent, the field value at which the effective potential turns negative (the so-called instability scale) is a gauge dependent quantity. By varying the gauge-fixing scheme and the gauge-fixing parameters in their perturbative domain, we find an irreducible theoretical uncertainty of at least two orders"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.7450","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":"2026-05-18T01:43:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcrHhaKnDzbwMuJEJd4xQq/yNeL9p6ACrc7rPrhMiaSUGR90AL+lV3LeX13XI3s2FNU3ROt8xzru9B6NFKZIBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T10:24:37.611526Z"},"content_sha256":"7fb14ccdf26953efd326183b3886f0abe29acaad4fe909f70851f40a088d40b8","schema_version":"1.0","event_id":"sha256:7fb14ccdf26953efd326183b3886f0abe29acaad4fe909f70851f40a088d40b8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/bundle.json","state_url":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/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":"2026-06-01T10:24:37Z","links":{"resolver":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W","bundle":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/bundle.json","state":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:CAIBUP4P2N7LE3C5RAFRHQID2W","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":"f6c87a59bb920b26a1a6defc2a924572a66edb9fa69dd0e432fa7fcd86dafbe1","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-29T18:21:12Z","title_canon_sha256":"8ed17630fe224dfe866f513537bd0417b1867bf9f82733e400dc40ad9254417f"},"schema_version":"1.0","source":{"id":"1404.7450","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.7450","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"arxiv_version","alias_value":"1404.7450v2","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7450","created_at":"2026-05-18T01:43:21Z"},{"alias_kind":"pith_short_12","alias_value":"CAIBUP4P2N7L","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_16","alias_value":"CAIBUP4P2N7LE3C5","created_at":"2026-05-18T12:28:22Z"},{"alias_kind":"pith_short_8","alias_value":"CAIBUP4P","created_at":"2026-05-18T12:28:22Z"}],"graph_snapshots":[{"event_id":"sha256:7fb14ccdf26953efd326183b3886f0abe29acaad4fe909f70851f40a088d40b8","target":"graph","created_at":"2026-05-18T01:43:21Z","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":"After reviewing the calculation of the Standard Model one-loop effective potential in a class of linear gauges, we discuss the physical observables entering the vacuum stability analysis. While the electroweak-vacuum-stability bound on the Higgs boson mass can be formally proven to be gauge independent, the field value at which the effective potential turns negative (the so-called instability scale) is a gauge dependent quantity. By varying the gauge-fixing scheme and the gauge-fixing parameters in their perturbative domain, we find an irreducible theoretical uncertainty of at least two orders","authors_text":"Luca Di Luzio, Luminita Mihaila","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-29T18:21:12Z","title":"On the gauge dependence of the Standard Model vacuum instability scale"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.7450","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:fdd4c20ae0b015b190434af5601913d718202c7933e8fe4cc0105ad3a7964ee2","target":"record","created_at":"2026-05-18T01:43:21Z","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":"f6c87a59bb920b26a1a6defc2a924572a66edb9fa69dd0e432fa7fcd86dafbe1","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-04-29T18:21:12Z","title_canon_sha256":"8ed17630fe224dfe866f513537bd0417b1867bf9f82733e400dc40ad9254417f"},"schema_version":"1.0","source":{"id":"1404.7450","kind":"arxiv","version":2}},"canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","first_computed_at":"2026-05-18T01:43:21.849181Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:43:21.849181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BcBdHWS6yHUHMAs0yVJgZCvdYXC66Iu4WQPBO6WEBu0N7X5OkyAXw9OaHU33HZQitOH+r/g3cmMvmERwuVTOBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:43:21.849809Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.7450","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fdd4c20ae0b015b190434af5601913d718202c7933e8fe4cc0105ad3a7964ee2","sha256:7fb14ccdf26953efd326183b3886f0abe29acaad4fe909f70851f40a088d40b8"],"state_sha256":"d997df829a41bb81b85b5b2e2c144a4a15d43372574aa99cb533eaa77050e13f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9aujJH723fSK1V873sLRupswbHQGpCnCyaYV0TOSn22XoJKb2BCSwVcZZfPRqXbqigQHixlMFhSpTH+UxnRYAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T10:24:37.613373Z","bundle_sha256":"df50220ccfe3e176bf2aae1edf5675f6f1303fcfeaad17a9564e912122e8e886"}}