{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:UNBLZZPPPRJMIPQJMMRTH42X2C","short_pith_number":"pith:UNBLZZPP","canonical_record":{"source":{"id":"hep-ph/9608350","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-08-16T17:35:14Z","cross_cats_sorted":[],"title_canon_sha256":"4ae0479916b00d60c6e41d35115eb9d09271c6ea3b32216c2cb008552eaf4975","abstract_canon_sha256":"ca60496b7c4492c9487149d120dd2b0ffa8b308fc6834f9ec004dfe10430459a"},"schema_version":"1.0"},"canonical_sha256":"a342bce5ef7c52c43e09632333f357d0b97a1f499f19e60e29245dd08881c84f","source":{"kind":"arxiv","id":"hep-ph/9608350","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9608350","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9608350v3","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9608350","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"pith_short_12","alias_value":"UNBLZZPPPRJM","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"UNBLZZPPPRJMIPQJ","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"UNBLZZPP","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:UNBLZZPPPRJMIPQJMMRTH42X2C","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9608350","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-08-16T17:35:14Z","cross_cats_sorted":[],"title_canon_sha256":"4ae0479916b00d60c6e41d35115eb9d09271c6ea3b32216c2cb008552eaf4975","abstract_canon_sha256":"ca60496b7c4492c9487149d120dd2b0ffa8b308fc6834f9ec004dfe10430459a"},"schema_version":"1.0"},"canonical_sha256":"a342bce5ef7c52c43e09632333f357d0b97a1f499f19e60e29245dd08881c84f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:23:55.104843Z","signature_b64":"kyCXPee4k76uR6ZD16Gv2Gtk9YwbBurJwxOryK9jJpi/iHF5oLPBZnAsfOB8PInL3AGTsfRuTqW7Suo+e7BfAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a342bce5ef7c52c43e09632333f357d0b97a1f499f19e60e29245dd08881c84f","last_reissued_at":"2026-05-18T04:23:55.104385Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:23:55.104385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9608350","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":"2026-05-18T04:23:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JJfOYxp+dxEs/MFBxmB8wQs6iAfJyExhKuTWhX1kCpw0bzh3k9LgMjoDq27l+DVmdjy9L7Gmw9jKwIA4t22DAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:53:06.165625Z"},"content_sha256":"54adef6933ea362663e6401becdd8220e0dad1c75bbcb4f6b0195830102b041e","schema_version":"1.0","event_id":"sha256:54adef6933ea362663e6401becdd8220e0dad1c75bbcb4f6b0195830102b041e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:UNBLZZPPPRJMIPQJMMRTH42X2C","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Classical Field Dynamics of the Electroweak Phase Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Guy D. Moore, Neil G. Turok","submitted_at":"1996-08-16T17:35:14Z","abstract_excerpt":"We investigate the thermodynamics and dynamics of the electroweak phase transition by modelling the infrared physics with classical Yang-Mills Higgs theory. We discuss the accuracy of this approach and conclude that, for quantities whose determination is dominated by the infrared, the classical method should be correct up to parametrically suppressed (ie O(alpha)) corrections. For a Higgs self-coupling which at tree level corresponds to m_H ~ 50 GeV, we determine the jump in the order parameter to be delta phi = 1.5 gT, the surface tension to be sigma = 0.07 g^4 T^3, and the friction coefficie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9608350","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":"2026-05-18T04:23:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Icpw6YLyfJOFuT6Bwimu5TdT9i6ETiYn4/xUe3tzkh3yQSQ39dZl9oneqWnGtj7pwB0V2yXleCvOwsBy46dyBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:53:06.165980Z"},"content_sha256":"f5f831131aad6245625698558b312a9281f3b806a57a9c963cd5e733d31f36a6","schema_version":"1.0","event_id":"sha256:f5f831131aad6245625698558b312a9281f3b806a57a9c963cd5e733d31f36a6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/bundle.json","state_url":"https://pith.science/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/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":"2026-05-30T06:53:06Z","links":{"resolver":"https://pith.science/pith/UNBLZZPPPRJMIPQJMMRTH42X2C","bundle":"https://pith.science/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/bundle.json","state":"https://pith.science/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UNBLZZPPPRJMIPQJMMRTH42X2C/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:UNBLZZPPPRJMIPQJMMRTH42X2C","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":"ca60496b7c4492c9487149d120dd2b0ffa8b308fc6834f9ec004dfe10430459a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-08-16T17:35:14Z","title_canon_sha256":"4ae0479916b00d60c6e41d35115eb9d09271c6ea3b32216c2cb008552eaf4975"},"schema_version":"1.0","source":{"id":"hep-ph/9608350","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9608350","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9608350v3","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9608350","created_at":"2026-05-18T04:23:55Z"},{"alias_kind":"pith_short_12","alias_value":"UNBLZZPPPRJM","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"UNBLZZPPPRJMIPQJ","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"UNBLZZPP","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:f5f831131aad6245625698558b312a9281f3b806a57a9c963cd5e733d31f36a6","target":"graph","created_at":"2026-05-18T04:23:55Z","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 thermodynamics and dynamics of the electroweak phase transition by modelling the infrared physics with classical Yang-Mills Higgs theory. We discuss the accuracy of this approach and conclude that, for quantities whose determination is dominated by the infrared, the classical method should be correct up to parametrically suppressed (ie O(alpha)) corrections. For a Higgs self-coupling which at tree level corresponds to m_H ~ 50 GeV, we determine the jump in the order parameter to be delta phi = 1.5 gT, the surface tension to be sigma = 0.07 g^4 T^3, and the friction coefficie","authors_text":"Guy D. Moore, Neil G. Turok","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1996-08-16T17:35:14Z","title":"Classical Field Dynamics of the Electroweak Phase Transition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9608350","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":"sha256:54adef6933ea362663e6401becdd8220e0dad1c75bbcb4f6b0195830102b041e","target":"record","created_at":"2026-05-18T04:23:55Z","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":"ca60496b7c4492c9487149d120dd2b0ffa8b308fc6834f9ec004dfe10430459a","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-08-16T17:35:14Z","title_canon_sha256":"4ae0479916b00d60c6e41d35115eb9d09271c6ea3b32216c2cb008552eaf4975"},"schema_version":"1.0","source":{"id":"hep-ph/9608350","kind":"arxiv","version":3}},"canonical_sha256":"a342bce5ef7c52c43e09632333f357d0b97a1f499f19e60e29245dd08881c84f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a342bce5ef7c52c43e09632333f357d0b97a1f499f19e60e29245dd08881c84f","first_computed_at":"2026-05-18T04:23:55.104385Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:23:55.104385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kyCXPee4k76uR6ZD16Gv2Gtk9YwbBurJwxOryK9jJpi/iHF5oLPBZnAsfOB8PInL3AGTsfRuTqW7Suo+e7BfAw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:23:55.104843Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9608350","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:54adef6933ea362663e6401becdd8220e0dad1c75bbcb4f6b0195830102b041e","sha256:f5f831131aad6245625698558b312a9281f3b806a57a9c963cd5e733d31f36a6"],"state_sha256":"05e6d8d72fdeebd009246f7a47d6ee89415272356584a7efa7666008897e70ad"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ntzOmge142QWcyxt7HTFbjyS/26d4XAZgPdN771AaUzo1IsZg3tNXhkXnSjnTavZurMuO0Hc5C8PiZFxVHqWBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:53:06.168050Z","bundle_sha256":"9e67a56ae464fead51511f9a5b002ce6318d71ccc93499f55eb6f6c2856cd3bb"}}