{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:KBSXRDA7FKGNFDAX32HYMB7EFM","short_pith_number":"pith:KBSXRDA7","canonical_record":{"source":{"id":"1710.07598","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-20T16:31:25Z","cross_cats_sorted":[],"title_canon_sha256":"46fc77e0413c24a0702f242bf0a2084a18a90e7bf9dcee4746569da82e12165e","abstract_canon_sha256":"bf9acf28a1ed6797a1d94ba36144c4fd61f0144d75c9f5f99769e9dee2cc63d5"},"schema_version":"1.0"},"canonical_sha256":"5065788c1f2a8cd28c17de8f8607e42b28f38146ebc62aabcdef37dea2704fb3","source":{"kind":"arxiv","id":"1710.07598","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.07598","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"arxiv_version","alias_value":"1710.07598v1","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07598","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"pith_short_12","alias_value":"KBSXRDA7FKGN","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KBSXRDA7FKGNFDAX","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KBSXRDA7","created_at":"2026-05-18T12:31:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:KBSXRDA7FKGNFDAX32HYMB7EFM","target":"record","payload":{"canonical_record":{"source":{"id":"1710.07598","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-20T16:31:25Z","cross_cats_sorted":[],"title_canon_sha256":"46fc77e0413c24a0702f242bf0a2084a18a90e7bf9dcee4746569da82e12165e","abstract_canon_sha256":"bf9acf28a1ed6797a1d94ba36144c4fd61f0144d75c9f5f99769e9dee2cc63d5"},"schema_version":"1.0"},"canonical_sha256":"5065788c1f2a8cd28c17de8f8607e42b28f38146ebc62aabcdef37dea2704fb3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:16.205901Z","signature_b64":"1iAZa2KSizs4Fb6oFK6TLAnnRXaMtLx1OhfLw1GOwpQIdDrJSlLgXvoLz33p2thCGDOU6Kdfaq/3WyhBBsbHAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5065788c1f2a8cd28c17de8f8607e42b28f38146ebc62aabcdef37dea2704fb3","last_reissued_at":"2026-05-18T00:18:16.205284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:16.205284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.07598","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":"2026-05-18T00:18:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Iyig6vf67N7TtEi+2AzHEd1OYQDzQ4FqsGtpdk1SnppAjMELWB/evtFcU+I2THrbMSQiU6602fZAOhGuJMZ1Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:42:49.431447Z"},"content_sha256":"c40cd1a0ae25b6e1843b00315120df0864b9b02ac923e14827480b2c28ead9bf","schema_version":"1.0","event_id":"sha256:c40cd1a0ae25b6e1843b00315120df0864b9b02ac923e14827480b2c28ead9bf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:KBSXRDA7FKGNFDAX32HYMB7EFM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Precision calculations for h->WW/ZZ->4 fermions in the Two-Higgs-Doublet Model with PROPHECY4F","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Heidi Rzehak, Lukas Altenkamp, Stefan Dittmaier","submitted_at":"2017-10-20T16:31:25Z","abstract_excerpt":"We have calculated the next-to-leading-order electroweak and QCD corrections to the decay processes h -> WW/ZZ -> 4 fermions of the light CP-even Higgs boson h of various types of Two-Higgs-Doublet Models (Types I and II, \"lepton-specific\" and \"flipped\" models). The input parameters are defined in four different renormalization schemes, where parameters that are not directly accessible by experiments are defined in the MSbar scheme. Numerical results are presented for the corrections to partial decay widths for various benchmark scenarios previously motivated in the literature, where we invest"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07598","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":"2026-05-18T00:18:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y6QCFV4FO+ScomLve+Wj4j+GJIcSuuy9xc5BJKs+BIGMcS5ZA93deYUD+e0pTlM7YcZkM79e+pcfDev0j8EUDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T21:42:49.431793Z"},"content_sha256":"0b8c26c51d6008de3cb562d2dccfd2ecb43ee15677becf6569155177fb840e9a","schema_version":"1.0","event_id":"sha256:0b8c26c51d6008de3cb562d2dccfd2ecb43ee15677becf6569155177fb840e9a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/bundle.json","state_url":"https://pith.science/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/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":"2026-06-02T21:42:49Z","links":{"resolver":"https://pith.science/pith/KBSXRDA7FKGNFDAX32HYMB7EFM","bundle":"https://pith.science/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/bundle.json","state":"https://pith.science/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KBSXRDA7FKGNFDAX32HYMB7EFM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:KBSXRDA7FKGNFDAX32HYMB7EFM","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":"bf9acf28a1ed6797a1d94ba36144c4fd61f0144d75c9f5f99769e9dee2cc63d5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-20T16:31:25Z","title_canon_sha256":"46fc77e0413c24a0702f242bf0a2084a18a90e7bf9dcee4746569da82e12165e"},"schema_version":"1.0","source":{"id":"1710.07598","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.07598","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"arxiv_version","alias_value":"1710.07598v1","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07598","created_at":"2026-05-18T00:18:16Z"},{"alias_kind":"pith_short_12","alias_value":"KBSXRDA7FKGN","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_16","alias_value":"KBSXRDA7FKGNFDAX","created_at":"2026-05-18T12:31:24Z"},{"alias_kind":"pith_short_8","alias_value":"KBSXRDA7","created_at":"2026-05-18T12:31:24Z"}],"graph_snapshots":[{"event_id":"sha256:0b8c26c51d6008de3cb562d2dccfd2ecb43ee15677becf6569155177fb840e9a","target":"graph","created_at":"2026-05-18T00:18:16Z","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 have calculated the next-to-leading-order electroweak and QCD corrections to the decay processes h -> WW/ZZ -> 4 fermions of the light CP-even Higgs boson h of various types of Two-Higgs-Doublet Models (Types I and II, \"lepton-specific\" and \"flipped\" models). The input parameters are defined in four different renormalization schemes, where parameters that are not directly accessible by experiments are defined in the MSbar scheme. Numerical results are presented for the corrections to partial decay widths for various benchmark scenarios previously motivated in the literature, where we invest","authors_text":"Heidi Rzehak, Lukas Altenkamp, Stefan Dittmaier","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-20T16:31:25Z","title":"Precision calculations for h->WW/ZZ->4 fermions in the Two-Higgs-Doublet Model with PROPHECY4F"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07598","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:c40cd1a0ae25b6e1843b00315120df0864b9b02ac923e14827480b2c28ead9bf","target":"record","created_at":"2026-05-18T00:18:16Z","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":"bf9acf28a1ed6797a1d94ba36144c4fd61f0144d75c9f5f99769e9dee2cc63d5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-20T16:31:25Z","title_canon_sha256":"46fc77e0413c24a0702f242bf0a2084a18a90e7bf9dcee4746569da82e12165e"},"schema_version":"1.0","source":{"id":"1710.07598","kind":"arxiv","version":1}},"canonical_sha256":"5065788c1f2a8cd28c17de8f8607e42b28f38146ebc62aabcdef37dea2704fb3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5065788c1f2a8cd28c17de8f8607e42b28f38146ebc62aabcdef37dea2704fb3","first_computed_at":"2026-05-18T00:18:16.205284Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:18:16.205284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1iAZa2KSizs4Fb6oFK6TLAnnRXaMtLx1OhfLw1GOwpQIdDrJSlLgXvoLz33p2thCGDOU6Kdfaq/3WyhBBsbHAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:18:16.205901Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.07598","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c40cd1a0ae25b6e1843b00315120df0864b9b02ac923e14827480b2c28ead9bf","sha256:0b8c26c51d6008de3cb562d2dccfd2ecb43ee15677becf6569155177fb840e9a"],"state_sha256":"038e1629de7f9ac3ba73a12727fa8e802b3bed9e2680a5b31907d63c52ea3478"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X/ob3p3aOTWUmSdc9gNcNkk0D6GlqNWmgd9f5W5mWSfMP9zGjSDTPXxxPhDjRZqyfmoOGXm1YAm9wpoDWoKMBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T21:42:49.433769Z","bundle_sha256":"d3239903711d5027750e880ab178875b6986408240f25ad76a933fa326f70246"}}