{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:S2X63CODB6LJNXP3SAG43AESMQ","short_pith_number":"pith:S2X63COD","canonical_record":{"source":{"id":"1808.01098","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-03T06:46:00Z","cross_cats_sorted":[],"title_canon_sha256":"16c0d926d32810a4d059057fb61ddeaf826b8fc904666e2fee5eeab83d50a94a","abstract_canon_sha256":"cfdd63e25adbd28494900b80c7bf783bc2d2df7b102bffbac88f10613a4f02ce"},"schema_version":"1.0"},"canonical_sha256":"96afed89c30f9696ddfb900dcd80926409f332811f004a9b70c9e45e183c0108","source":{"kind":"arxiv","id":"1808.01098","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.01098","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"arxiv_version","alias_value":"1808.01098v2","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.01098","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"pith_short_12","alias_value":"S2X63CODB6LJ","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"S2X63CODB6LJNXP3","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"S2X63COD","created_at":"2026-05-18T12:32:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:S2X63CODB6LJNXP3SAG43AESMQ","target":"record","payload":{"canonical_record":{"source":{"id":"1808.01098","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-03T06:46:00Z","cross_cats_sorted":[],"title_canon_sha256":"16c0d926d32810a4d059057fb61ddeaf826b8fc904666e2fee5eeab83d50a94a","abstract_canon_sha256":"cfdd63e25adbd28494900b80c7bf783bc2d2df7b102bffbac88f10613a4f02ce"},"schema_version":"1.0"},"canonical_sha256":"96afed89c30f9696ddfb900dcd80926409f332811f004a9b70c9e45e183c0108","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:04.262650Z","signature_b64":"qu8pdmXO3SZib1djDZSMpBNwFZe7Dm6D9H66r4YBHAw05K4p5g1gJYrYf182p/YoX5eyZ8You0oh5xD1YUqMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"96afed89c30f9696ddfb900dcd80926409f332811f004a9b70c9e45e183c0108","last_reissued_at":"2026-05-17T23:58:04.262131Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:04.262131Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1808.01098","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":"2026-05-17T23:58:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8v7S/Nx/RHUgpb27zyehCSCpTWqWIA3uYiQIcPDhkVhSGzFMlbr5Jtn4bc4OuDPGB3Ho2w2re46EE/f7/Fh6Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:10:29.684258Z"},"content_sha256":"8c22c5246b81b88590873b36adce9235277923b346eb47c8024ef7bf9265f9a0","schema_version":"1.0","event_id":"sha256:8c22c5246b81b88590873b36adce9235277923b346eb47c8024ef7bf9265f9a0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:S2X63CODB6LJNXP3SAG43AESMQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Revisiting electroweak phase transition in the standard model with a real singlet scalar","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng-Wei Chiang, Eibun Senaha, Yen-Ting Li","submitted_at":"2018-08-03T06:46:00Z","abstract_excerpt":"We revisit the electroweak phase transition in the standard model with a real scalar, utilizing several calculation methods to investigate scheme dependences. We quantify the numerical impacts of Nambu-Goldstone resummation, required in one of the schemes, on the strength of the first-order electroweak phase transition. We also employ a gauge-independent scheme to make a comparison with the standard gauge-dependent results. It is found that the effect of the Nambu-Goldstone resummation is typically $\\sim1\\%$. Our analysis shows that both gauge-dependent and -independent methods give qualitativ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.01098","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":"2026-05-17T23:58:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KPb/WXyovMMFQfPzTbomlAKPygNhMfkd/BA4ryNo3wzt9w8SNcNlkGvsNKe6CD55g1/DBjJHZ+jZPPffks2ECw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:10:29.685072Z"},"content_sha256":"c0e14eef04d8661ea078627f15670ddd69243a22027dcdeb8bc2edb4dbfbe98d","schema_version":"1.0","event_id":"sha256:c0e14eef04d8661ea078627f15670ddd69243a22027dcdeb8bc2edb4dbfbe98d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/S2X63CODB6LJNXP3SAG43AESMQ/bundle.json","state_url":"https://pith.science/pith/S2X63CODB6LJNXP3SAG43AESMQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/S2X63CODB6LJNXP3SAG43AESMQ/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":"2026-05-27T07:10:29Z","links":{"resolver":"https://pith.science/pith/S2X63CODB6LJNXP3SAG43AESMQ","bundle":"https://pith.science/pith/S2X63CODB6LJNXP3SAG43AESMQ/bundle.json","state":"https://pith.science/pith/S2X63CODB6LJNXP3SAG43AESMQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/S2X63CODB6LJNXP3SAG43AESMQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:S2X63CODB6LJNXP3SAG43AESMQ","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":"cfdd63e25adbd28494900b80c7bf783bc2d2df7b102bffbac88f10613a4f02ce","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-03T06:46:00Z","title_canon_sha256":"16c0d926d32810a4d059057fb61ddeaf826b8fc904666e2fee5eeab83d50a94a"},"schema_version":"1.0","source":{"id":"1808.01098","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1808.01098","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"arxiv_version","alias_value":"1808.01098v2","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1808.01098","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"pith_short_12","alias_value":"S2X63CODB6LJ","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"S2X63CODB6LJNXP3","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"S2X63COD","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:c0e14eef04d8661ea078627f15670ddd69243a22027dcdeb8bc2edb4dbfbe98d","target":"graph","created_at":"2026-05-17T23:58:04Z","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 revisit the electroweak phase transition in the standard model with a real scalar, utilizing several calculation methods to investigate scheme dependences. We quantify the numerical impacts of Nambu-Goldstone resummation, required in one of the schemes, on the strength of the first-order electroweak phase transition. We also employ a gauge-independent scheme to make a comparison with the standard gauge-dependent results. It is found that the effect of the Nambu-Goldstone resummation is typically $\\sim1\\%$. Our analysis shows that both gauge-dependent and -independent methods give qualitativ","authors_text":"Cheng-Wei Chiang, Eibun Senaha, Yen-Ting Li","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-03T06:46:00Z","title":"Revisiting electroweak phase transition in the standard model with a real singlet scalar"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1808.01098","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":"sha256:8c22c5246b81b88590873b36adce9235277923b346eb47c8024ef7bf9265f9a0","target":"record","created_at":"2026-05-17T23:58:04Z","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":"cfdd63e25adbd28494900b80c7bf783bc2d2df7b102bffbac88f10613a4f02ce","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-08-03T06:46:00Z","title_canon_sha256":"16c0d926d32810a4d059057fb61ddeaf826b8fc904666e2fee5eeab83d50a94a"},"schema_version":"1.0","source":{"id":"1808.01098","kind":"arxiv","version":2}},"canonical_sha256":"96afed89c30f9696ddfb900dcd80926409f332811f004a9b70c9e45e183c0108","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"96afed89c30f9696ddfb900dcd80926409f332811f004a9b70c9e45e183c0108","first_computed_at":"2026-05-17T23:58:04.262131Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:58:04.262131Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"qu8pdmXO3SZib1djDZSMpBNwFZe7Dm6D9H66r4YBHAw05K4p5g1gJYrYf182p/YoX5eyZ8You0oh5xD1YUqMCw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:58:04.262650Z","signed_message":"canonical_sha256_bytes"},"source_id":"1808.01098","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8c22c5246b81b88590873b36adce9235277923b346eb47c8024ef7bf9265f9a0","sha256:c0e14eef04d8661ea078627f15670ddd69243a22027dcdeb8bc2edb4dbfbe98d"],"state_sha256":"328989be2ed34405a215da234c9009d350a417d3ac7446b6ac6649cc4242ef46"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pTDRdOOGwL40aS1ehl57/crZJb/C94kwmdJlpY6G8UrP0q5CJljRMLw/ma1Z46SBrgJ19nKqUctkqfc0maSoBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T07:10:29.688992Z","bundle_sha256":"cfb8121c98c5873513327e8776fcbc37876eee5c75d0e45c55ede21a27873571"}}