{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:YPF3XLC3E7KT2A7NDTKH6BWFGU","short_pith_number":"pith:YPF3XLC3","canonical_record":{"source":{"id":"1602.00695","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-01T21:00:05Z","cross_cats_sorted":[],"title_canon_sha256":"93e2409b2ec5062dace75352a308e03e8c1bd782f044ef15d68cde5e785de71d","abstract_canon_sha256":"0e7afa0f243738936d72f5498e453aaf398132f76e1e72c612383e7173b2f771"},"schema_version":"1.0"},"canonical_sha256":"c3cbbbac5b27d53d03ed1cd47f06c53525557b60a15c7c4002fc8f68b24fdfec","source":{"kind":"arxiv","id":"1602.00695","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00695","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00695v1","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00695","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"pith_short_12","alias_value":"YPF3XLC3E7KT","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YPF3XLC3E7KT2A7N","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YPF3XLC3","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:YPF3XLC3E7KT2A7NDTKH6BWFGU","target":"record","payload":{"canonical_record":{"source":{"id":"1602.00695","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-01T21:00:05Z","cross_cats_sorted":[],"title_canon_sha256":"93e2409b2ec5062dace75352a308e03e8c1bd782f044ef15d68cde5e785de71d","abstract_canon_sha256":"0e7afa0f243738936d72f5498e453aaf398132f76e1e72c612383e7173b2f771"},"schema_version":"1.0"},"canonical_sha256":"c3cbbbac5b27d53d03ed1cd47f06c53525557b60a15c7c4002fc8f68b24fdfec","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:24.897733Z","signature_b64":"SCRVl/NfLEzd4yu94TRUoZnoxSO4YuVfIeEvOP3boTNac1NODG1mIeyj2QdATTtGo7/Vk7wlTjaRVfW04ZTFCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3cbbbac5b27d53d03ed1cd47f06c53525557b60a15c7c4002fc8f68b24fdfec","last_reissued_at":"2026-05-18T01:21:24.897181Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:24.897181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.00695","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":"2026-05-18T01:21:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uxE/0x28Gb5ZNEb/KEu4W7Zfm+ogCvtjcj5/AGB5AptCTTRWceWAYqNgNr6BxFbNsdR2RLAVLRMBrNdgVf0PDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:07:23.458284Z"},"content_sha256":"bba4f1eaf41d6abc208ff6aba6f544c79831e819f7d1d8a19e53cbd5e65b9b73","schema_version":"1.0","event_id":"sha256:bba4f1eaf41d6abc208ff6aba6f544c79831e819f7d1d8a19e53cbd5e65b9b73"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:YPF3XLC3E7KT2A7NDTKH6BWFGU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High precision determination of the gluon fusion Higgs boson cross-section at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Achilleas Lazopoulos, Bernhard Mistlberger, Charalampos Anastasiou, Claude Duhr, Elisabetta Furlan, Falko Dulat, Franz Herzog, Thomas Gehrmann","submitted_at":"2016-02-01T21:00:05Z","abstract_excerpt":"We present the most precise value for the Higgs boson cross-section in the gluon-fusion production mode at the LHC. Our result is based on a perturbative expansion through N$^3$LO in QCD, in an effective theory where the top-quark is assumed to be infinitely heavy, while all other Standard Model quarks are massless. We combine this result with QCD corrections to the cross-section where all finite quark-mass effects are included exactly through NLO. In addition, electroweak corrections and the first corrections in the inverse mass of the top-quark are incorporated at three loops. We also invest"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00695","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":"2026-05-18T01:21:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hwicf7xVKqJSRxTOo2W7MV7DUVM7Ht3G/W1Uim3HzUwFCdM9UW2/yY4kneCbUl8pvBjbmW4OU+T1aDsWmDiTDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T00:07:23.458672Z"},"content_sha256":"ebb915bcadf05847400dad9de1918882c2f452937e5a32454e8de869516b331a","schema_version":"1.0","event_id":"sha256:ebb915bcadf05847400dad9de1918882c2f452937e5a32454e8de869516b331a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/bundle.json","state_url":"https://pith.science/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/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":"2026-05-26T00:07:23Z","links":{"resolver":"https://pith.science/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU","bundle":"https://pith.science/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/bundle.json","state":"https://pith.science/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YPF3XLC3E7KT2A7NDTKH6BWFGU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:YPF3XLC3E7KT2A7NDTKH6BWFGU","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":"0e7afa0f243738936d72f5498e453aaf398132f76e1e72c612383e7173b2f771","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-01T21:00:05Z","title_canon_sha256":"93e2409b2ec5062dace75352a308e03e8c1bd782f044ef15d68cde5e785de71d"},"schema_version":"1.0","source":{"id":"1602.00695","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.00695","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"arxiv_version","alias_value":"1602.00695v1","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.00695","created_at":"2026-05-18T01:21:24Z"},{"alias_kind":"pith_short_12","alias_value":"YPF3XLC3E7KT","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YPF3XLC3E7KT2A7N","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YPF3XLC3","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:ebb915bcadf05847400dad9de1918882c2f452937e5a32454e8de869516b331a","target":"graph","created_at":"2026-05-18T01:21:24Z","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 present the most precise value for the Higgs boson cross-section in the gluon-fusion production mode at the LHC. Our result is based on a perturbative expansion through N$^3$LO in QCD, in an effective theory where the top-quark is assumed to be infinitely heavy, while all other Standard Model quarks are massless. We combine this result with QCD corrections to the cross-section where all finite quark-mass effects are included exactly through NLO. In addition, electroweak corrections and the first corrections in the inverse mass of the top-quark are incorporated at three loops. We also invest","authors_text":"Achilleas Lazopoulos, Bernhard Mistlberger, Charalampos Anastasiou, Claude Duhr, Elisabetta Furlan, Falko Dulat, Franz Herzog, Thomas Gehrmann","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-01T21:00:05Z","title":"High precision determination of the gluon fusion Higgs boson cross-section at the LHC"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.00695","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:bba4f1eaf41d6abc208ff6aba6f544c79831e819f7d1d8a19e53cbd5e65b9b73","target":"record","created_at":"2026-05-18T01:21:24Z","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":"0e7afa0f243738936d72f5498e453aaf398132f76e1e72c612383e7173b2f771","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-01T21:00:05Z","title_canon_sha256":"93e2409b2ec5062dace75352a308e03e8c1bd782f044ef15d68cde5e785de71d"},"schema_version":"1.0","source":{"id":"1602.00695","kind":"arxiv","version":1}},"canonical_sha256":"c3cbbbac5b27d53d03ed1cd47f06c53525557b60a15c7c4002fc8f68b24fdfec","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3cbbbac5b27d53d03ed1cd47f06c53525557b60a15c7c4002fc8f68b24fdfec","first_computed_at":"2026-05-18T01:21:24.897181Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:21:24.897181Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"SCRVl/NfLEzd4yu94TRUoZnoxSO4YuVfIeEvOP3boTNac1NODG1mIeyj2QdATTtGo7/Vk7wlTjaRVfW04ZTFCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:21:24.897733Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.00695","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bba4f1eaf41d6abc208ff6aba6f544c79831e819f7d1d8a19e53cbd5e65b9b73","sha256:ebb915bcadf05847400dad9de1918882c2f452937e5a32454e8de869516b331a"],"state_sha256":"94b82c5e03217d39f6b31fb16f5fb2a74b7d96e0d485e0539a000e6550247c5a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Yv+q8n1B9S/hc22NVWt/QYJx8Xn4RJtwdv518PBMddnMk2SdbPMsfEwkoDnBB8rrxVFqXO5z/6L8lYrcokZvCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T00:07:23.460961Z","bundle_sha256":"2951790cb8a0b9d71111427b159b6e6b45515c56929a9aa3cac9583605f8dde2"}}