{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:HC2GX7FS3TTTFE4ADN44PN4CCA","short_pith_number":"pith:HC2GX7FS","schema_version":"1.0","canonical_sha256":"38b46bfcb2dce73293801b79c7b782101082cb0b862503c924035671a8dcc3f2","source":{"kind":"arxiv","id":"2402.02914","version":3},"attestation_state":"computed","paper":{"title":"Feasibility of ultrarelativistic bubbles in SMEFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Sabyasachi Chakraborty, Shakeel Ur Rahaman, Suraj Prakash, Upalaparna Banerjee","submitted_at":"2024-02-05T11:30:04Z","abstract_excerpt":"A first order electroweak phase transition probes physics beyond the Standard Model on multiple frontiers and therefore is of immense interest for theoretical exploration. We conduct a model-independent study of the effects of relevant dimension 6 and dimension 8 operators, of the Standard Model effective field theory, on electroweak phase transition. We use a thermally corrected and renormalization group improved potential and study its impact on nucleation temperature. We then outline bubble dynamics that lead to ultrarelativistic bubble wall velocities which are mainly motivated from the vi"},"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":"2402.02914","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-05T11:30:04Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"91b4b5e6579cca84f50ee3426f1664e17e9a26cd640fc667dc8cdff2fd517453","abstract_canon_sha256":"9f673b67665a93d55ef246080175be2a9beaba1428555628113fd5adf53e40d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:56:16.930503Z","signature_b64":"weFwlyHp6Qt8+OiZVD0Io31CFay3yAT+qbqL2rS/072tbkxyToIqacpzMRts3J3wEGAL055fH84f4oRkwRLDBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38b46bfcb2dce73293801b79c7b782101082cb0b862503c924035671a8dcc3f2","last_reissued_at":"2026-07-05T08:56:16.930085Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:56:16.930085Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Feasibility of ultrarelativistic bubbles in SMEFT","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Sabyasachi Chakraborty, Shakeel Ur Rahaman, Suraj Prakash, Upalaparna Banerjee","submitted_at":"2024-02-05T11:30:04Z","abstract_excerpt":"A first order electroweak phase transition probes physics beyond the Standard Model on multiple frontiers and therefore is of immense interest for theoretical exploration. We conduct a model-independent study of the effects of relevant dimension 6 and dimension 8 operators, of the Standard Model effective field theory, on electroweak phase transition. We use a thermally corrected and renormalization group improved potential and study its impact on nucleation temperature. We then outline bubble dynamics that lead to ultrarelativistic bubble wall velocities which are mainly motivated from the vi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.02914","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2402.02914/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2402.02914","created_at":"2026-07-05T08:56:16.930140+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.02914v3","created_at":"2026-07-05T08:56:16.930140+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.02914","created_at":"2026-07-05T08:56:16.930140+00:00"},{"alias_kind":"pith_short_12","alias_value":"HC2GX7FS3TTT","created_at":"2026-07-05T08:56:16.930140+00:00"},{"alias_kind":"pith_short_16","alias_value":"HC2GX7FS3TTTFE4A","created_at":"2026-07-05T08:56:16.930140+00:00"},{"alias_kind":"pith_short_8","alias_value":"HC2GX7FS","created_at":"2026-07-05T08:56:16.930140+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.30740","citing_title":"Dynamical evolution of the pressure on the bubble wall","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2603.18583","citing_title":"Electroweak phase transitions in a $U(1)_D$ extension of the standard model with dimension-six operators: Gravitational waves and LHC signatures","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA","json":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA.json","graph_json":"https://pith.science/api/pith-number/HC2GX7FS3TTTFE4ADN44PN4CCA/graph.json","events_json":"https://pith.science/api/pith-number/HC2GX7FS3TTTFE4ADN44PN4CCA/events.json","paper":"https://pith.science/paper/HC2GX7FS"},"agent_actions":{"view_html":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA","download_json":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA.json","view_paper":"https://pith.science/paper/HC2GX7FS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.02914&json=true","fetch_graph":"https://pith.science/api/pith-number/HC2GX7FS3TTTFE4ADN44PN4CCA/graph.json","fetch_events":"https://pith.science/api/pith-number/HC2GX7FS3TTTFE4ADN44PN4CCA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA/action/storage_attestation","attest_author":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA/action/author_attestation","sign_citation":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA/action/citation_signature","submit_replication":"https://pith.science/pith/HC2GX7FS3TTTFE4ADN44PN4CCA/action/replication_record"}},"created_at":"2026-07-05T08:56:16.930140+00:00","updated_at":"2026-07-05T08:56:16.930140+00:00"}