{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:5FGBCBEZSJI6IHTP4VCWNW5I4H","short_pith_number":"pith:5FGBCBEZ","canonical_record":{"source":{"id":"hep-lat/9702017","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1997-02-20T16:36:08Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"92bb30888cd7cea405414809ef282c91513e3c69b99077f1a28bd2001542d154","abstract_canon_sha256":"903348cb73dded1df3c9a75deefa4384a042816488e7c49e06655fd735fbe09c"},"schema_version":"1.0"},"canonical_sha256":"e94c1104999251e41e6fe54566dba8e1eadef0ac67f2978cfb47a1159791346d","source":{"kind":"arxiv","id":"hep-lat/9702017","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9702017","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9702017v2","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9702017","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"pith_short_12","alias_value":"5FGBCBEZSJI6","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"5FGBCBEZSJI6IHTP","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"5FGBCBEZ","created_at":"2026-05-18T12:25:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:5FGBCBEZSJI6IHTP4VCWNW5I4H","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/9702017","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1997-02-20T16:36:08Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"92bb30888cd7cea405414809ef282c91513e3c69b99077f1a28bd2001542d154","abstract_canon_sha256":"903348cb73dded1df3c9a75deefa4384a042816488e7c49e06655fd735fbe09c"},"schema_version":"1.0"},"canonical_sha256":"e94c1104999251e41e6fe54566dba8e1eadef0ac67f2978cfb47a1159791346d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:13.226935Z","signature_b64":"tXqD46iq9zW6/3Br9leqpYus3dHpzF6IMbdLwM8Nu3EFAvBotEsepJIrcjn3m3SAh8Xum8GARuGRh+sB37jlBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e94c1104999251e41e6fe54566dba8e1eadef0ac67f2978cfb47a1159791346d","last_reissued_at":"2026-05-18T01:39:13.226231Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:13.226231Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/9702017","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":"2026-05-18T01:39:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i5Vfi5t7f+qENx+pyAMrfgCEcterNa2opgCFZz5qeBfZklkvxkXcSf0gES4WOEtXo6GYO0TwMwLRXRA0NLgXAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:13:46.371112Z"},"content_sha256":"95ce6b2d622a4b4f48a1590249633430e472e49e594cb5a990955e206b6d82d7","schema_version":"1.0","event_id":"sha256:95ce6b2d622a4b4f48a1590249633430e472e49e594cb5a990955e206b6d82d7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:5FGBCBEZSJI6IHTP4VCWNW5I4H","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Numerical study of plasmon properties in the SU(2)-Higgs model","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"J. Smit, W.H. Tang","submitted_at":"1997-02-20T16:36:08Z","abstract_excerpt":"Using the (effective) classical approximation, we compute numerically time-dependent correlation functions in the SU(2)-Higgs model around the electroweak phase transition, for $m_H \\approx m_W$. The parameters of the classical model have been determined previously by the dimensional reduction relations for time-independent correlators. The $H$ and $W$ correlation functions correspond to gauge invariant fields. They show damped oscillatory behavior from which we extract frequencies $\\om$ and damping rates $\\gm$. In the Higgs phase the damping rates have roughly the values obtained in analytic "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9702017","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":"2026-05-18T01:39:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9xialQjSNQ/3W6HD8IkqlBoMOD8oU2UbXg6oQk10JDHiAOPVS8M/Xgr653oEMT8uZwMqwrDu3OTuZkkojWmDBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:13:46.371495Z"},"content_sha256":"cd2a58db9c293083eb32a7c9a3967a22684874aa3e5e8c1a365e1e249b09eeb2","schema_version":"1.0","event_id":"sha256:cd2a58db9c293083eb32a7c9a3967a22684874aa3e5e8c1a365e1e249b09eeb2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/bundle.json","state_url":"https://pith.science/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/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":"2026-05-31T03:13:46Z","links":{"resolver":"https://pith.science/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H","bundle":"https://pith.science/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/bundle.json","state":"https://pith.science/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5FGBCBEZSJI6IHTP4VCWNW5I4H/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:5FGBCBEZSJI6IHTP4VCWNW5I4H","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":"903348cb73dded1df3c9a75deefa4384a042816488e7c49e06655fd735fbe09c","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"1997-02-20T16:36:08Z","title_canon_sha256":"92bb30888cd7cea405414809ef282c91513e3c69b99077f1a28bd2001542d154"},"schema_version":"1.0","source":{"id":"hep-lat/9702017","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9702017","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9702017v2","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9702017","created_at":"2026-05-18T01:39:13Z"},{"alias_kind":"pith_short_12","alias_value":"5FGBCBEZSJI6","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_16","alias_value":"5FGBCBEZSJI6IHTP","created_at":"2026-05-18T12:25:48Z"},{"alias_kind":"pith_short_8","alias_value":"5FGBCBEZ","created_at":"2026-05-18T12:25:48Z"}],"graph_snapshots":[{"event_id":"sha256:cd2a58db9c293083eb32a7c9a3967a22684874aa3e5e8c1a365e1e249b09eeb2","target":"graph","created_at":"2026-05-18T01:39:13Z","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":"Using the (effective) classical approximation, we compute numerically time-dependent correlation functions in the SU(2)-Higgs model around the electroweak phase transition, for $m_H \\approx m_W$. The parameters of the classical model have been determined previously by the dimensional reduction relations for time-independent correlators. The $H$ and $W$ correlation functions correspond to gauge invariant fields. They show damped oscillatory behavior from which we extract frequencies $\\om$ and damping rates $\\gm$. In the Higgs phase the damping rates have roughly the values obtained in analytic ","authors_text":"J. Smit, W.H. Tang","cross_cats":["hep-ph"],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1997-02-20T16:36:08Z","title":"Numerical study of plasmon properties in the SU(2)-Higgs model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9702017","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":"sha256:95ce6b2d622a4b4f48a1590249633430e472e49e594cb5a990955e206b6d82d7","target":"record","created_at":"2026-05-18T01:39:13Z","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":"903348cb73dded1df3c9a75deefa4384a042816488e7c49e06655fd735fbe09c","cross_cats_sorted":["hep-ph"],"license":"","primary_cat":"hep-lat","submitted_at":"1997-02-20T16:36:08Z","title_canon_sha256":"92bb30888cd7cea405414809ef282c91513e3c69b99077f1a28bd2001542d154"},"schema_version":"1.0","source":{"id":"hep-lat/9702017","kind":"arxiv","version":2}},"canonical_sha256":"e94c1104999251e41e6fe54566dba8e1eadef0ac67f2978cfb47a1159791346d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e94c1104999251e41e6fe54566dba8e1eadef0ac67f2978cfb47a1159791346d","first_computed_at":"2026-05-18T01:39:13.226231Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:13.226231Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tXqD46iq9zW6/3Br9leqpYus3dHpzF6IMbdLwM8Nu3EFAvBotEsepJIrcjn3m3SAh8Xum8GARuGRh+sB37jlBw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:13.226935Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9702017","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:95ce6b2d622a4b4f48a1590249633430e472e49e594cb5a990955e206b6d82d7","sha256:cd2a58db9c293083eb32a7c9a3967a22684874aa3e5e8c1a365e1e249b09eeb2"],"state_sha256":"04c8152eedbb3da96ecedc37ac7d9a3e07f0e4dd5cd8a42b1ececcc12561b077"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NCSY03+dJbp6/O6UPmVBapZl98PKAJ2odzxcgRCm4s2NbJhYqb+QyYAh2gObXaqC0WIFiV703CYZK674dKQ7AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T03:13:46.373456Z","bundle_sha256":"14fb7d55380ab633cf590f79b5530fe4e0d6d937d37f05730419932b963710b5"}}