{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:QWVY54UYMET6ET5WGBUJMP7UWG","short_pith_number":"pith:QWVY54UY","canonical_record":{"source":{"id":"0911.0687","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-11-03T21:03:14Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"d68e354f504e825afa9d681924e799cc59f0dfb711a2951a9efae6a7e23f32e9","abstract_canon_sha256":"e6c986613c264eeebf042101d28619bd52b5ed069d0ef2ca13b2b02871b7c38c"},"schema_version":"1.0"},"canonical_sha256":"85ab8ef2986127e24fb63068963ff4b1a1dee3cc90e45eebaa7ad25babdba953","source":{"kind":"arxiv","id":"0911.0687","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0911.0687","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"arxiv_version","alias_value":"0911.0687v3","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0911.0687","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"pith_short_12","alias_value":"QWVY54UYMET6","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"QWVY54UYMET6ET5W","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"QWVY54UY","created_at":"2026-05-18T12:26:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:QWVY54UYMET6ET5WGBUJMP7UWG","target":"record","payload":{"canonical_record":{"source":{"id":"0911.0687","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-11-03T21:03:14Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"d68e354f504e825afa9d681924e799cc59f0dfb711a2951a9efae6a7e23f32e9","abstract_canon_sha256":"e6c986613c264eeebf042101d28619bd52b5ed069d0ef2ca13b2b02871b7c38c"},"schema_version":"1.0"},"canonical_sha256":"85ab8ef2986127e24fb63068963ff4b1a1dee3cc90e45eebaa7ad25babdba953","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:11.998799Z","signature_b64":"U6JjARUWXjzfdu/db/IJng1I1TlXJZi3uNl6PwmMR4QUhJ7MIgzXU7KwSXm0c48pO9B49cnHPDLQE03XxAK5Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"85ab8ef2986127e24fb63068963ff4b1a1dee3cc90e45eebaa7ad25babdba953","last_reissued_at":"2026-05-18T02:34:11.995361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:11.995361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0911.0687","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:34:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"En2tIc4MzXIhIMA0VngWBokkcvy+xyKoxsk4mVXOfRNvZE0nQ+cgeFeEh6i0wxogpWLX2a7scynDvdV8CCsvAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T04:41:26.917909Z"},"content_sha256":"527f974f3e8f03a66717eada0b402afb0ce014079038691fe232c85a80fd97ce","schema_version":"1.0","event_id":"sha256:527f974f3e8f03a66717eada0b402afb0ce014079038691fe232c85a80fd97ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:QWVY54UYMET6ET5WGBUJMP7UWG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Semi-Analytic Calculation of the Gravitational Wave Signal From the Electroweak Phase Transition for General Quartic Scalar Effective Potentials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"hep-ph","authors_text":"John Kehayias, Stefano Profumo","submitted_at":"2009-11-03T21:03:14Z","abstract_excerpt":"Upcoming gravitational wave (GW) detectors might detect a stochastic background of GWs potentially arising from many possible sources, including bubble collisions from a strongly first-order electroweak phase transition. We investigate whether it is possible to connect, via a semi-analytical approximation to the tunneling rate of scalar fields with quartic potentials, the GW signal through detonations with the parameters entering the potential that drives the electroweak phase transition. To this end, we consider a finite temperature effective potential similar in form to the Higgs potential i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0911.0687","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":""},"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":"2026-05-18T02:34:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qovp9LB15sTWa9CNdvNI3NJZ+p72+1vbLtIyLDW1p49IJgk1DoG9kfwpGXWZ5TvrnpS1v9DlVuOjebs9ed4JAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T04:41:26.918249Z"},"content_sha256":"d993c31ba1147023ea635d3a8654c9709ebc4beb2ee6b269bfecb73ee509e451","schema_version":"1.0","event_id":"sha256:d993c31ba1147023ea635d3a8654c9709ebc4beb2ee6b269bfecb73ee509e451"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/QWVY54UYMET6ET5WGBUJMP7UWG/bundle.json","state_url":"https://pith.science/pith/QWVY54UYMET6ET5WGBUJMP7UWG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/QWVY54UYMET6ET5WGBUJMP7UWG/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":"2026-07-05T04:41:26Z","links":{"resolver":"https://pith.science/pith/QWVY54UYMET6ET5WGBUJMP7UWG","bundle":"https://pith.science/pith/QWVY54UYMET6ET5WGBUJMP7UWG/bundle.json","state":"https://pith.science/pith/QWVY54UYMET6ET5WGBUJMP7UWG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/QWVY54UYMET6ET5WGBUJMP7UWG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:QWVY54UYMET6ET5WGBUJMP7UWG","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":"e6c986613c264eeebf042101d28619bd52b5ed069d0ef2ca13b2b02871b7c38c","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-11-03T21:03:14Z","title_canon_sha256":"d68e354f504e825afa9d681924e799cc59f0dfb711a2951a9efae6a7e23f32e9"},"schema_version":"1.0","source":{"id":"0911.0687","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0911.0687","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"arxiv_version","alias_value":"0911.0687v3","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0911.0687","created_at":"2026-05-18T02:34:11Z"},{"alias_kind":"pith_short_12","alias_value":"QWVY54UYMET6","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"QWVY54UYMET6ET5W","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"QWVY54UY","created_at":"2026-05-18T12:26:01Z"}],"graph_snapshots":[{"event_id":"sha256:d993c31ba1147023ea635d3a8654c9709ebc4beb2ee6b269bfecb73ee509e451","target":"graph","created_at":"2026-05-18T02:34:11Z","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":"Upcoming gravitational wave (GW) detectors might detect a stochastic background of GWs potentially arising from many possible sources, including bubble collisions from a strongly first-order electroweak phase transition. We investigate whether it is possible to connect, via a semi-analytical approximation to the tunneling rate of scalar fields with quartic potentials, the GW signal through detonations with the parameters entering the potential that drives the electroweak phase transition. To this end, we consider a finite temperature effective potential similar in form to the Higgs potential i","authors_text":"John Kehayias, Stefano Profumo","cross_cats":["astro-ph.CO","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-11-03T21:03:14Z","title":"Semi-Analytic Calculation of the Gravitational Wave Signal From the Electroweak Phase Transition for General Quartic Scalar Effective Potentials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0911.0687","kind":"arxiv","version":3},"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":"sha256:527f974f3e8f03a66717eada0b402afb0ce014079038691fe232c85a80fd97ce","target":"record","created_at":"2026-05-18T02:34:11Z","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":"e6c986613c264eeebf042101d28619bd52b5ed069d0ef2ca13b2b02871b7c38c","cross_cats_sorted":["astro-ph.CO","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-11-03T21:03:14Z","title_canon_sha256":"d68e354f504e825afa9d681924e799cc59f0dfb711a2951a9efae6a7e23f32e9"},"schema_version":"1.0","source":{"id":"0911.0687","kind":"arxiv","version":3}},"canonical_sha256":"85ab8ef2986127e24fb63068963ff4b1a1dee3cc90e45eebaa7ad25babdba953","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"85ab8ef2986127e24fb63068963ff4b1a1dee3cc90e45eebaa7ad25babdba953","first_computed_at":"2026-05-18T02:34:11.995361Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:34:11.995361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"U6JjARUWXjzfdu/db/IJng1I1TlXJZi3uNl6PwmMR4QUhJ7MIgzXU7KwSXm0c48pO9B49cnHPDLQE03XxAK5Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:34:11.998799Z","signed_message":"canonical_sha256_bytes"},"source_id":"0911.0687","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:527f974f3e8f03a66717eada0b402afb0ce014079038691fe232c85a80fd97ce","sha256:d993c31ba1147023ea635d3a8654c9709ebc4beb2ee6b269bfecb73ee509e451"],"state_sha256":"bcd40bc6f2d67f6a6a50a3d95aef74218340cfd58be51786c492033c4ddae8e9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"A0A0rVItBP9z6gv4K0v2kDdWnD6foEycxxR1SAk3dOlmkAUkRxH+ea4D6Ag6+O2sRbZWUUV+G5Ob57+pwoh8Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T04:41:26.920224Z","bundle_sha256":"db749b913dd002fcd38d9fba531495a06422c4c53f667939a0194ec459cfc800"}}