{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:ZTRUPYJXPTR5KEAFJGXOKXUHBL","short_pith_number":"pith:ZTRUPYJX","canonical_record":{"source":{"id":"1809.04994","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-13T14:45:02Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"34f712619b79a3578aee7a3b70587354647df3044b047a95c83dc5648ed20505","abstract_canon_sha256":"128eaa3d7208df51edf3d3faf745bd7fce6c25ea7ad77f19b19b687c8e5f8468"},"schema_version":"1.0"},"canonical_sha256":"cce347e1377ce3d5100549aee55e870acd20f2bd3aa3a559f9ef6c7da948de42","source":{"kind":"arxiv","id":"1809.04994","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.04994","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"arxiv_version","alias_value":"1809.04994v1","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.04994","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"pith_short_12","alias_value":"ZTRUPYJXPTR5","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZTRUPYJXPTR5KEAF","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZTRUPYJX","created_at":"2026-05-18T12:33:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:ZTRUPYJXPTR5KEAFJGXOKXUHBL","target":"record","payload":{"canonical_record":{"source":{"id":"1809.04994","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-13T14:45:02Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"34f712619b79a3578aee7a3b70587354647df3044b047a95c83dc5648ed20505","abstract_canon_sha256":"128eaa3d7208df51edf3d3faf745bd7fce6c25ea7ad77f19b19b687c8e5f8468"},"schema_version":"1.0"},"canonical_sha256":"cce347e1377ce3d5100549aee55e870acd20f2bd3aa3a559f9ef6c7da948de42","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:48:33.836941Z","signature_b64":"wKx7WNI+rdme5f/Vd97ysCohcnBAg4JhtKhKfev/X+A+Kq6XIh4UlnaIFJyTBvnc+44W34roNhg5RqIV5G76Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cce347e1377ce3d5100549aee55e870acd20f2bd3aa3a559f9ef6c7da948de42","last_reissued_at":"2026-05-17T23:48:33.836301Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:48:33.836301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1809.04994","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:48:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H9fN/kyORroTw5bzIeO3/E3PNC6G8Mdz+40ZJ9xCY27nkDFfJw+N3sEdmb+DME9aFX4S8N6ORo2haZBUve2zCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:08:48.432263Z"},"content_sha256":"b4a85db67c6bb64d2c40a19f96589d35ec600949d1c361fa4f9a49865f3411ff","schema_version":"1.0","event_id":"sha256:b4a85db67c6bb64d2c40a19f96589d35ec600949d1c361fa4f9a49865f3411ff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:ZTRUPYJXPTR5KEAFJGXOKXUHBL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fingerprinting models of first-order phase transitions by the synergy between collider and gravitational-wave experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Katsuya Hashino, Masahiro Takimoto, Mitsuru Kakizaki, Ryusuke Jinno, Shinya Kanemura, Tomo Takahashi","submitted_at":"2018-09-13T14:45:02Z","abstract_excerpt":"We investigate the sensitivity of future space-based interferometers such as LISA and DECIGO to the parameters of new particle physics models which drive a first-order phase transition in the early Universe. We first perform a Fisher matrix analysis on the quantities characterizing the gravitational wave spectrum resulting from the phase transition, such as the peak frequency and amplitude. We next perform a Fisher analysis for the quantities which determine the properties of the phase transition, such as the latent heat and the time dependence of the bubble nucleation rate. Since these quanti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.04994","kind":"arxiv","version":1},"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":"2026-05-17T23:48:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZW95o3sn0pd9xjcGiQjsJkMlCkgJ8UqOWagkoljoWaxtbhjY6R68F8gUuj3QJVNAw0I8gUhw7gcyYcY1lxqaAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T11:08:48.432643Z"},"content_sha256":"9bd4c832e2aff92a408fbf212a3dd48c7ddcf20970cca1c48e727d2aea4ee38e","schema_version":"1.0","event_id":"sha256:9bd4c832e2aff92a408fbf212a3dd48c7ddcf20970cca1c48e727d2aea4ee38e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/bundle.json","state_url":"https://pith.science/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/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":"2026-05-30T11:08:48Z","links":{"resolver":"https://pith.science/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL","bundle":"https://pith.science/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/bundle.json","state":"https://pith.science/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZTRUPYJXPTR5KEAFJGXOKXUHBL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ZTRUPYJXPTR5KEAFJGXOKXUHBL","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":"128eaa3d7208df51edf3d3faf745bd7fce6c25ea7ad77f19b19b687c8e5f8468","cross_cats_sorted":["astro-ph.CO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-13T14:45:02Z","title_canon_sha256":"34f712619b79a3578aee7a3b70587354647df3044b047a95c83dc5648ed20505"},"schema_version":"1.0","source":{"id":"1809.04994","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.04994","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"arxiv_version","alias_value":"1809.04994v1","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.04994","created_at":"2026-05-17T23:48:33Z"},{"alias_kind":"pith_short_12","alias_value":"ZTRUPYJXPTR5","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZTRUPYJXPTR5KEAF","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZTRUPYJX","created_at":"2026-05-18T12:33:07Z"}],"graph_snapshots":[{"event_id":"sha256:9bd4c832e2aff92a408fbf212a3dd48c7ddcf20970cca1c48e727d2aea4ee38e","target":"graph","created_at":"2026-05-17T23:48:33Z","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 investigate the sensitivity of future space-based interferometers such as LISA and DECIGO to the parameters of new particle physics models which drive a first-order phase transition in the early Universe. We first perform a Fisher matrix analysis on the quantities characterizing the gravitational wave spectrum resulting from the phase transition, such as the peak frequency and amplitude. We next perform a Fisher analysis for the quantities which determine the properties of the phase transition, such as the latent heat and the time dependence of the bubble nucleation rate. Since these quanti","authors_text":"Katsuya Hashino, Masahiro Takimoto, Mitsuru Kakizaki, Ryusuke Jinno, Shinya Kanemura, Tomo Takahashi","cross_cats":["astro-ph.CO"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-13T14:45:02Z","title":"Fingerprinting models of first-order phase transitions by the synergy between collider and gravitational-wave experiments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.04994","kind":"arxiv","version":1},"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:b4a85db67c6bb64d2c40a19f96589d35ec600949d1c361fa4f9a49865f3411ff","target":"record","created_at":"2026-05-17T23:48:33Z","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":"128eaa3d7208df51edf3d3faf745bd7fce6c25ea7ad77f19b19b687c8e5f8468","cross_cats_sorted":["astro-ph.CO"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-13T14:45:02Z","title_canon_sha256":"34f712619b79a3578aee7a3b70587354647df3044b047a95c83dc5648ed20505"},"schema_version":"1.0","source":{"id":"1809.04994","kind":"arxiv","version":1}},"canonical_sha256":"cce347e1377ce3d5100549aee55e870acd20f2bd3aa3a559f9ef6c7da948de42","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cce347e1377ce3d5100549aee55e870acd20f2bd3aa3a559f9ef6c7da948de42","first_computed_at":"2026-05-17T23:48:33.836301Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:48:33.836301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wKx7WNI+rdme5f/Vd97ysCohcnBAg4JhtKhKfev/X+A+Kq6XIh4UlnaIFJyTBvnc+44W34roNhg5RqIV5G76Cg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:48:33.836941Z","signed_message":"canonical_sha256_bytes"},"source_id":"1809.04994","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b4a85db67c6bb64d2c40a19f96589d35ec600949d1c361fa4f9a49865f3411ff","sha256:9bd4c832e2aff92a408fbf212a3dd48c7ddcf20970cca1c48e727d2aea4ee38e"],"state_sha256":"e45d3203c317ad33fc0438135b26d58b0677b60b5d195ae3a9a4ae01834abdfe"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nO/a0iInfKofIJD0V5pHenx5s52TAbT+cEJPUohn5xV3cw2heQqEITv94G3Hdyv9QV89fPQQrjKSF9keUO3xDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T11:08:48.434748Z","bundle_sha256":"c666d627bc429b65845382c51269521ca3ed1ca0d30915b0f56c9856f396ecbb"}}