{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:CAIBUP4P2N7LE3C5RAFRHQID2W","short_pith_number":"pith:CAIBUP4P","schema_version":"1.0","canonical_sha256":"10101a3f8fd37eb26c5d880b13c103d5a4db077a72d9e2f2b4cda2d3fdbafee8","source":{"kind":"arxiv","id":"1404.7450","version":2},"attestation_state":"computed","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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"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"},"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"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1404.7450","created_at":"2026-05-18T01:43:21.849273+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.7450v2","created_at":"2026-05-18T01:43:21.849273+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.7450","created_at":"2026-05-18T01:43:21.849273+00:00"},{"alias_kind":"pith_short_12","alias_value":"CAIBUP4P2N7L","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"CAIBUP4P2N7LE3C5","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"CAIBUP4P","created_at":"2026-05-18T12:28:22.404517+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.05972","citing_title":"Background Fields Meet the Heat Kernel: Gauge Invariance and RGEs without diagrams","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W","json":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W.json","graph_json":"https://pith.science/api/pith-number/CAIBUP4P2N7LE3C5RAFRHQID2W/graph.json","events_json":"https://pith.science/api/pith-number/CAIBUP4P2N7LE3C5RAFRHQID2W/events.json","paper":"https://pith.science/paper/CAIBUP4P"},"agent_actions":{"view_html":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W","download_json":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W.json","view_paper":"https://pith.science/paper/CAIBUP4P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.7450&json=true","fetch_graph":"https://pith.science/api/pith-number/CAIBUP4P2N7LE3C5RAFRHQID2W/graph.json","fetch_events":"https://pith.science/api/pith-number/CAIBUP4P2N7LE3C5RAFRHQID2W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/action/storage_attestation","attest_author":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/action/author_attestation","sign_citation":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/action/citation_signature","submit_replication":"https://pith.science/pith/CAIBUP4P2N7LE3C5RAFRHQID2W/action/replication_record"}},"created_at":"2026-05-18T01:43:21.849273+00:00","updated_at":"2026-05-18T01:43:21.849273+00:00"}