{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:YO35AUXOFFUDUMW76HHJGSY7RF","short_pith_number":"pith:YO35AUXO","canonical_record":{"source":{"id":"1509.08394","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T17:07:03Z","cross_cats_sorted":[],"title_canon_sha256":"4c05ce929f3ee117eeb23c7d029c7d20b8eed021e3c31f0a11128d4425bf3bb9","abstract_canon_sha256":"afa2c7edb3c9ec0d5218d0747329a40b1866e465676f2287aa0bfc6da2994329"},"schema_version":"1.0"},"canonical_sha256":"c3b7d052ee29683a32dff1ce934b1f894b8f7fa9a55d4ff842ae774b3eb16a0a","source":{"kind":"arxiv","id":"1509.08394","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08394","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08394v2","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08394","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"pith_short_12","alias_value":"YO35AUXOFFUD","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"YO35AUXOFFUDUMW7","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"YO35AUXO","created_at":"2026-05-18T12:29:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:YO35AUXOFFUDUMW76HHJGSY7RF","target":"record","payload":{"canonical_record":{"source":{"id":"1509.08394","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T17:07:03Z","cross_cats_sorted":[],"title_canon_sha256":"4c05ce929f3ee117eeb23c7d029c7d20b8eed021e3c31f0a11128d4425bf3bb9","abstract_canon_sha256":"afa2c7edb3c9ec0d5218d0747329a40b1866e465676f2287aa0bfc6da2994329"},"schema_version":"1.0"},"canonical_sha256":"c3b7d052ee29683a32dff1ce934b1f894b8f7fa9a55d4ff842ae774b3eb16a0a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:18.200051Z","signature_b64":"GkIebSujt+/fCoett3VdmSBllj0PCOWcSKnxwz5HVJ/WXbNwCM8UGruEMkRSLWE4xDYuK6OeEIstgfQrceVpBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3b7d052ee29683a32dff1ce934b1f894b8f7fa9a55d4ff842ae774b3eb16a0a","last_reissued_at":"2026-05-18T01:24:18.199519Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:18.199519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1509.08394","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":"2026-05-18T01:24:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V1TsWBAExPnEIWyk/KzHVBGMzw+cmdXiZSKJwMBTSFgNvmG1egDjX7LYZ843jb0YDnzKKGyV6I8h+Ke0fWEXDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T15:39:38.512495Z"},"content_sha256":"a7a003564e584d0254fdb0cbcc94a649e65a06cf4dd08ba65a42957c05eea5f3","schema_version":"1.0","event_id":"sha256:a7a003564e584d0254fdb0cbcc94a649e65a06cf4dd08ba65a42957c05eea5f3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:YO35AUXOFFUDUMW76HHJGSY7RF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Gravitational waves as a probe of extended scalar sectors with the first order electroweak phase transition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mitsuru Kakizaki, Shinya Kanemura, Toshinori Matsui","submitted_at":"2015-09-28T17:07:03Z","abstract_excerpt":"We discuss spectra of gravitational waves which are originated by the strongly first order phase transition at the electroweak symmetry breaking, which is required for a successful scenario of electroweak baryogenesis. Such spectra are numerically evaluated without high temperature expansion in a set of extended scalar sectors with additional N isospin-singlet fields as a concrete example of renormalizable theories. We find that the produced gravitational waves can be significant, so that they are detectable at future gravitational wave interferometers such as DECIGO and BBO. Furthermore, sinc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08394","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":"2026-05-18T01:24:18Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DVZhmbtH+fI/kwvvtFiqtEUJtMwIvG7VzqxysuCRhqRuq8b3uWU4V71wdX8b+o40VqT29C8TZBEfNIr1cL7DCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T15:39:38.513146Z"},"content_sha256":"7031f647397b9c57e71ccd5e812ec87ccda17451c2a6e5d6c633d621587f918f","schema_version":"1.0","event_id":"sha256:7031f647397b9c57e71ccd5e812ec87ccda17451c2a6e5d6c633d621587f918f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YO35AUXOFFUDUMW76HHJGSY7RF/bundle.json","state_url":"https://pith.science/pith/YO35AUXOFFUDUMW76HHJGSY7RF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YO35AUXOFFUDUMW76HHJGSY7RF/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":"2026-05-30T15:39:38Z","links":{"resolver":"https://pith.science/pith/YO35AUXOFFUDUMW76HHJGSY7RF","bundle":"https://pith.science/pith/YO35AUXOFFUDUMW76HHJGSY7RF/bundle.json","state":"https://pith.science/pith/YO35AUXOFFUDUMW76HHJGSY7RF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YO35AUXOFFUDUMW76HHJGSY7RF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:YO35AUXOFFUDUMW76HHJGSY7RF","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":"afa2c7edb3c9ec0d5218d0747329a40b1866e465676f2287aa0bfc6da2994329","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T17:07:03Z","title_canon_sha256":"4c05ce929f3ee117eeb23c7d029c7d20b8eed021e3c31f0a11128d4425bf3bb9"},"schema_version":"1.0","source":{"id":"1509.08394","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1509.08394","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"arxiv_version","alias_value":"1509.08394v2","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08394","created_at":"2026-05-18T01:24:18Z"},{"alias_kind":"pith_short_12","alias_value":"YO35AUXOFFUD","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"YO35AUXOFFUDUMW7","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"YO35AUXO","created_at":"2026-05-18T12:29:50Z"}],"graph_snapshots":[{"event_id":"sha256:7031f647397b9c57e71ccd5e812ec87ccda17451c2a6e5d6c633d621587f918f","target":"graph","created_at":"2026-05-18T01:24:18Z","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 discuss spectra of gravitational waves which are originated by the strongly first order phase transition at the electroweak symmetry breaking, which is required for a successful scenario of electroweak baryogenesis. Such spectra are numerically evaluated without high temperature expansion in a set of extended scalar sectors with additional N isospin-singlet fields as a concrete example of renormalizable theories. We find that the produced gravitational waves can be significant, so that they are detectable at future gravitational wave interferometers such as DECIGO and BBO. Furthermore, sinc","authors_text":"Mitsuru Kakizaki, Shinya Kanemura, Toshinori Matsui","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T17:07:03Z","title":"Gravitational waves as a probe of extended scalar sectors with the first order electroweak phase transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08394","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:a7a003564e584d0254fdb0cbcc94a649e65a06cf4dd08ba65a42957c05eea5f3","target":"record","created_at":"2026-05-18T01:24:18Z","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":"afa2c7edb3c9ec0d5218d0747329a40b1866e465676f2287aa0bfc6da2994329","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-09-28T17:07:03Z","title_canon_sha256":"4c05ce929f3ee117eeb23c7d029c7d20b8eed021e3c31f0a11128d4425bf3bb9"},"schema_version":"1.0","source":{"id":"1509.08394","kind":"arxiv","version":2}},"canonical_sha256":"c3b7d052ee29683a32dff1ce934b1f894b8f7fa9a55d4ff842ae774b3eb16a0a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3b7d052ee29683a32dff1ce934b1f894b8f7fa9a55d4ff842ae774b3eb16a0a","first_computed_at":"2026-05-18T01:24:18.199519Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:24:18.199519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GkIebSujt+/fCoett3VdmSBllj0PCOWcSKnxwz5HVJ/WXbNwCM8UGruEMkRSLWE4xDYuK6OeEIstgfQrceVpBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:24:18.200051Z","signed_message":"canonical_sha256_bytes"},"source_id":"1509.08394","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a7a003564e584d0254fdb0cbcc94a649e65a06cf4dd08ba65a42957c05eea5f3","sha256:7031f647397b9c57e71ccd5e812ec87ccda17451c2a6e5d6c633d621587f918f"],"state_sha256":"713a374db175a28ab8eedb643f22deebc61b68293d328c8d466ba52eb2987215"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bJh8fvx8DnyE286Pqw5HU4LvWaF+1v5f+Njo3oLGg7HQibVSy7e7pcSHSeOLyMtjwVlTqIqMqIhLTLXhsUCbAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T15:39:38.516545Z","bundle_sha256":"794adbf831b6995ad5332ce0c418b3da79c11e18f1fe6c6f121e6f100b92fc35"}}