{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:NW3QPZ6AHZM5BGR3Y4DNVKHEJF","short_pith_number":"pith:NW3QPZ6A","canonical_record":{"source":{"id":"hep-ph/9804255","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-08T09:29:36Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"555cddb496d5e1387eb421a89d2d822a0671ca324aba9629b9296ab756c568e8","abstract_canon_sha256":"45b10dccbbf3d3c7e883cb92f97ba879356a3f8f54a8a7b066542f5810fd3786"},"schema_version":"1.0"},"canonical_sha256":"6db707e7c03e59d09a3bc706daa8e4495ab81d745392e2104299c0eb752a34cd","source":{"kind":"arxiv","id":"hep-ph/9804255","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9804255","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9804255v1","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9804255","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"pith_short_12","alias_value":"NW3QPZ6AHZM5","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"NW3QPZ6AHZM5BGR3","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"NW3QPZ6A","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:NW3QPZ6AHZM5BGR3Y4DNVKHEJF","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9804255","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-08T09:29:36Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"555cddb496d5e1387eb421a89d2d822a0671ca324aba9629b9296ab756c568e8","abstract_canon_sha256":"45b10dccbbf3d3c7e883cb92f97ba879356a3f8f54a8a7b066542f5810fd3786"},"schema_version":"1.0"},"canonical_sha256":"6db707e7c03e59d09a3bc706daa8e4495ab81d745392e2104299c0eb752a34cd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:50.612340Z","signature_b64":"5ILMuUyD7MvP/ck55R+1GqrVMGdpt1wfO0O/Y4cg8ufzccJzTebYc3aB744H9t0R5nCBmi0xU+TPzrvJ1mWMDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6db707e7c03e59d09a3bc706daa8e4495ab81d745392e2104299c0eb752a34cd","last_reissued_at":"2026-05-18T04:22:50.611750Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:50.611750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9804255","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":"2026-05-18T04:22:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QTw5BRw3vD9QYoIPZftJmFX9M7mX4Uv2k+/m5OZaeVIulc9jxytPqiy47DbeQ5AKf81m9y/cWbCLcvJ3nZHHAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T11:40:03.356905Z"},"content_sha256":"328c5cac2995eb332385fd6fb11649dd12430577dd21a96ab3cfef832e5c9899","schema_version":"1.0","event_id":"sha256:328c5cac2995eb332385fd6fb11649dd12430577dd21a96ab3cfef832e5c9899"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:NW3QPZ6AHZM5BGR3Y4DNVKHEJF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A Strong Electroweak Phase Transition up to m_H ~ 105 GeV","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"(2) NORDITA), K. Rummukainen (2) ((1) CERN, M. Laine (1)","submitted_at":"1998-04-08T09:29:36Z","abstract_excerpt":"Non-perturbative lattice simulations have shown that there is no electroweak phase transition in the Standard Model for the allowed Higgs masses, m_H \\gsim 75 GeV. In the Minimal Supersymmetric Standard Model, in contrast, it has been proposed that the transition should exist and even be strong enough for baryogenesis up to m_H ~ 105 GeV, provided that the lightest stop mass is in the range 100...160 GeV. However, this prediction is based on perturbation theory, and suffers from a noticeable gauge parameter and renormalization scale dependence. We have performed large-scale lattice Monte Carlo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9804255","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":"2026-05-18T04:22:50Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fl+ThsmlhpubMr0P7yyomw17wALjIYJNJQEenIWqnO0xNVoKhO5Tw3OkiGomEEJedHNHwPYAfL3ofFfzeXbxBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-30T11:40:03.357239Z"},"content_sha256":"f40d73f02e23ad06c9aeb1cdaf77d62aa6d9c77e36a66071fa0834532cc194b2","schema_version":"1.0","event_id":"sha256:f40d73f02e23ad06c9aeb1cdaf77d62aa6d9c77e36a66071fa0834532cc194b2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/bundle.json","state_url":"https://pith.science/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/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":"2026-06-30T11:40:03Z","links":{"resolver":"https://pith.science/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF","bundle":"https://pith.science/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/bundle.json","state":"https://pith.science/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NW3QPZ6AHZM5BGR3Y4DNVKHEJF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:NW3QPZ6AHZM5BGR3Y4DNVKHEJF","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":"45b10dccbbf3d3c7e883cb92f97ba879356a3f8f54a8a7b066542f5810fd3786","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-08T09:29:36Z","title_canon_sha256":"555cddb496d5e1387eb421a89d2d822a0671ca324aba9629b9296ab756c568e8"},"schema_version":"1.0","source":{"id":"hep-ph/9804255","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9804255","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9804255v1","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9804255","created_at":"2026-05-18T04:22:50Z"},{"alias_kind":"pith_short_12","alias_value":"NW3QPZ6AHZM5","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"NW3QPZ6AHZM5BGR3","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"NW3QPZ6A","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:f40d73f02e23ad06c9aeb1cdaf77d62aa6d9c77e36a66071fa0834532cc194b2","target":"graph","created_at":"2026-05-18T04:22:50Z","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":"Non-perturbative lattice simulations have shown that there is no electroweak phase transition in the Standard Model for the allowed Higgs masses, m_H \\gsim 75 GeV. In the Minimal Supersymmetric Standard Model, in contrast, it has been proposed that the transition should exist and even be strong enough for baryogenesis up to m_H ~ 105 GeV, provided that the lightest stop mass is in the range 100...160 GeV. However, this prediction is based on perturbation theory, and suffers from a noticeable gauge parameter and renormalization scale dependence. We have performed large-scale lattice Monte Carlo","authors_text":"(2) NORDITA), K. Rummukainen (2) ((1) CERN, M. Laine (1)","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1998-04-08T09:29:36Z","title":"A Strong Electroweak Phase Transition up to m_H ~ 105 GeV"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9804255","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":"sha256:328c5cac2995eb332385fd6fb11649dd12430577dd21a96ab3cfef832e5c9899","target":"record","created_at":"2026-05-18T04:22:50Z","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":"45b10dccbbf3d3c7e883cb92f97ba879356a3f8f54a8a7b066542f5810fd3786","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1998-04-08T09:29:36Z","title_canon_sha256":"555cddb496d5e1387eb421a89d2d822a0671ca324aba9629b9296ab756c568e8"},"schema_version":"1.0","source":{"id":"hep-ph/9804255","kind":"arxiv","version":1}},"canonical_sha256":"6db707e7c03e59d09a3bc706daa8e4495ab81d745392e2104299c0eb752a34cd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6db707e7c03e59d09a3bc706daa8e4495ab81d745392e2104299c0eb752a34cd","first_computed_at":"2026-05-18T04:22:50.611750Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:22:50.611750Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5ILMuUyD7MvP/ck55R+1GqrVMGdpt1wfO0O/Y4cg8ufzccJzTebYc3aB744H9t0R5nCBmi0xU+TPzrvJ1mWMDA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:22:50.612340Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9804255","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:328c5cac2995eb332385fd6fb11649dd12430577dd21a96ab3cfef832e5c9899","sha256:f40d73f02e23ad06c9aeb1cdaf77d62aa6d9c77e36a66071fa0834532cc194b2"],"state_sha256":"f2279b356ebf714b5eb9d35cf55ca319f2ad3611f39214a8d37dc55312059239"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T0XVU7Ra59nusub4VY2FgVw+Nr1z77xRteMFS55J1nDK3Qt+RzkrOmUyTmD4kAPx1B3YffZHw6+487dJmSjFDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-30T11:40:03.359076Z","bundle_sha256":"aab2fc76709ee1ca373c19f88fc4fbbd76a7aa5eea73d43d2e8048dceb1609c9"}}