{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:RTUSGCLL34XDDZ6SRAFKYUCVMG","short_pith_number":"pith:RTUSGCLL","canonical_record":{"source":{"id":"2403.03769","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-06T15:04:31Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"421b09e116ccff9910d136cfe1ee4c600f69315aba5578fb63781ead0ee3821e","abstract_canon_sha256":"a2826a13f4a6ddb38c8fe4c24f6290c0d2798f74ffd78435fcedc7467ee4ab0c"},"schema_version":"1.0"},"canonical_sha256":"8ce923096bdf2e31e7d2880aac5055619a8886ac2c8a3dd1ec9653bbe1411e13","source":{"kind":"arxiv","id":"2403.03769","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.03769","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"arxiv_version","alias_value":"2403.03769v2","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.03769","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_12","alias_value":"RTUSGCLL34XD","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_16","alias_value":"RTUSGCLL34XDDZ6S","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_8","alias_value":"RTUSGCLL","created_at":"2026-07-05T10:52:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:RTUSGCLL34XDDZ6SRAFKYUCVMG","target":"record","payload":{"canonical_record":{"source":{"id":"2403.03769","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-06T15:04:31Z","cross_cats_sorted":["astro-ph.CO"],"title_canon_sha256":"421b09e116ccff9910d136cfe1ee4c600f69315aba5578fb63781ead0ee3821e","abstract_canon_sha256":"a2826a13f4a6ddb38c8fe4c24f6290c0d2798f74ffd78435fcedc7467ee4ab0c"},"schema_version":"1.0"},"canonical_sha256":"8ce923096bdf2e31e7d2880aac5055619a8886ac2c8a3dd1ec9653bbe1411e13","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:52:54.040922Z","signature_b64":"xquwG5ohnywkmwU9JkNndsqetMZYS1qGe5bu/MFGZDGGJYd3cL2F1uwyBgCP4XB3C9Pzo5NzjVDcpma372p5CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8ce923096bdf2e31e7d2880aac5055619a8886ac2c8a3dd1ec9653bbe1411e13","last_reissued_at":"2026-07-05T10:52:54.040486Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:52:54.040486Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2403.03769","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":"2026-07-05T10:52:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"48hz7RUaU7RgpYWDVcGzOO7TjS4tq8gFuek9ZUTyFUiE7mIaDvVCrdFRCChceTCA29NrxPlCCGq0fG110YLvCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T23:05:51.696191Z"},"content_sha256":"adfa70aaa590ca9f441e3360af5b4f086f5511a6a0159b52ff9cdcf821dbce0a","schema_version":"1.0","event_id":"sha256:adfa70aaa590ca9f441e3360af5b4f086f5511a6a0159b52ff9cdcf821dbce0a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:RTUSGCLL34XDDZ6SRAFKYUCVMG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Impact of theoretical uncertainties on model parameter reconstruction from GW signals sourced by cosmological phase transitions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO"],"primary_cat":"hep-ph","authors_text":"Daniel Schmitt, Laura Sagunski, Marco Merchand, Marek Lewicki, Philipp Schicho","submitted_at":"2024-03-06T15:04:31Z","abstract_excerpt":"Different computational techniques for cosmological phase transition parameters can impact the Gravitational Wave (GW) spectra predicted in a given particle physics model. To scrutinize the importance of this effect, we perform large-scale parameter scans of the dynamical real-singlet extended Standard Model using three perturbative approximations for the effective potential: the $\\overline{\\rm MS}$ and on-shell schemes at leading order, and three-dimensional thermal effective theory (3D EFT) at next-to-leading order. While predictions of GW amplitudes are typically unreliable in the absence o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.03769","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2403.03769/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:52:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3igTnXSPdkHGZMkXRZ8JfnclrM16F+Dn/VFlXY93zGVbgLzeSfz1mbhH+mCEiFfoS9P7P5rFWQG4kULFLsi3Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T23:05:51.696725Z"},"content_sha256":"d434c85032b1fa8e1b9aa9cd2eafdbfd1d833ecd73695188cacad6feb646736e","schema_version":"1.0","event_id":"sha256:d434c85032b1fa8e1b9aa9cd2eafdbfd1d833ecd73695188cacad6feb646736e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/bundle.json","state_url":"https://pith.science/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/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":"2026-08-09T23:05:51Z","links":{"resolver":"https://pith.science/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG","bundle":"https://pith.science/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/bundle.json","state":"https://pith.science/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RTUSGCLL34XDDZ6SRAFKYUCVMG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:RTUSGCLL34XDDZ6SRAFKYUCVMG","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":"a2826a13f4a6ddb38c8fe4c24f6290c0d2798f74ffd78435fcedc7467ee4ab0c","cross_cats_sorted":["astro-ph.CO"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-06T15:04:31Z","title_canon_sha256":"421b09e116ccff9910d136cfe1ee4c600f69315aba5578fb63781ead0ee3821e"},"schema_version":"1.0","source":{"id":"2403.03769","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.03769","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"arxiv_version","alias_value":"2403.03769v2","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.03769","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_12","alias_value":"RTUSGCLL34XD","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_16","alias_value":"RTUSGCLL34XDDZ6S","created_at":"2026-07-05T10:52:54Z"},{"alias_kind":"pith_short_8","alias_value":"RTUSGCLL","created_at":"2026-07-05T10:52:54Z"}],"graph_snapshots":[{"event_id":"sha256:d434c85032b1fa8e1b9aa9cd2eafdbfd1d833ecd73695188cacad6feb646736e","target":"graph","created_at":"2026-07-05T10:52:54Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2403.03769/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Different computational techniques for cosmological phase transition parameters can impact the Gravitational Wave (GW) spectra predicted in a given particle physics model. To scrutinize the importance of this effect, we perform large-scale parameter scans of the dynamical real-singlet extended Standard Model using three perturbative approximations for the effective potential: the $\\overline{\\rm MS}$ and on-shell schemes at leading order, and three-dimensional thermal effective theory (3D EFT) at next-to-leading order. While predictions of GW amplitudes are typically unreliable in the absence o","authors_text":"Daniel Schmitt, Laura Sagunski, Marco Merchand, Marek Lewicki, Philipp Schicho","cross_cats":["astro-ph.CO"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-06T15:04:31Z","title":"Impact of theoretical uncertainties on model parameter reconstruction from GW signals sourced by cosmological phase transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.03769","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:adfa70aaa590ca9f441e3360af5b4f086f5511a6a0159b52ff9cdcf821dbce0a","target":"record","created_at":"2026-07-05T10:52:54Z","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":"a2826a13f4a6ddb38c8fe4c24f6290c0d2798f74ffd78435fcedc7467ee4ab0c","cross_cats_sorted":["astro-ph.CO"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-03-06T15:04:31Z","title_canon_sha256":"421b09e116ccff9910d136cfe1ee4c600f69315aba5578fb63781ead0ee3821e"},"schema_version":"1.0","source":{"id":"2403.03769","kind":"arxiv","version":2}},"canonical_sha256":"8ce923096bdf2e31e7d2880aac5055619a8886ac2c8a3dd1ec9653bbe1411e13","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8ce923096bdf2e31e7d2880aac5055619a8886ac2c8a3dd1ec9653bbe1411e13","first_computed_at":"2026-07-05T10:52:54.040486Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:52:54.040486Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xquwG5ohnywkmwU9JkNndsqetMZYS1qGe5bu/MFGZDGGJYd3cL2F1uwyBgCP4XB3C9Pzo5NzjVDcpma372p5CQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:52:54.040922Z","signed_message":"canonical_sha256_bytes"},"source_id":"2403.03769","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:adfa70aaa590ca9f441e3360af5b4f086f5511a6a0159b52ff9cdcf821dbce0a","sha256:d434c85032b1fa8e1b9aa9cd2eafdbfd1d833ecd73695188cacad6feb646736e"],"state_sha256":"070afab5d1d9a778c64fb0b15b8a2c0ed01f97b899aaa99bbeeb3841d4d38af5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IvD4rX5lZ6jezGbiS0hC2kq5C43/WWhnvCgVyzKd1SBgbwIMPeASR/nfgK2CLjggemaX9/3JWocd00GU947vDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T23:05:51.702806Z","bundle_sha256":"ce76b8267229f7af2cada5e15ffb8175700d4a2f9b4645c3e19b15be634791d0"}}