{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:OLSWWDEMK6TMJS52DROVVNRAF5","short_pith_number":"pith:OLSWWDEM","canonical_record":{"source":{"id":"1106.4250","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-06-21T16:16:02Z","cross_cats_sorted":[],"title_canon_sha256":"7ad2bdb26cb58bb8a00d524fd110de2c7ee317f48b2181e2255e943d6a7fa326","abstract_canon_sha256":"afa586619ad50b9e38e98500bf681316736d8ec81308f92207ebfad94de2b3d8"},"schema_version":"1.0"},"canonical_sha256":"72e56b0c8c57a6c4cbba1c5d5ab6202f73508767f15889ddc6c9302f5a79c413","source":{"kind":"arxiv","id":"1106.4250","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.4250","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"arxiv_version","alias_value":"1106.4250v2","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.4250","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"pith_short_12","alias_value":"OLSWWDEMK6TM","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"OLSWWDEMK6TMJS52","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"OLSWWDEM","created_at":"2026-05-18T12:26:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:OLSWWDEMK6TMJS52DROVVNRAF5","target":"record","payload":{"canonical_record":{"source":{"id":"1106.4250","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-06-21T16:16:02Z","cross_cats_sorted":[],"title_canon_sha256":"7ad2bdb26cb58bb8a00d524fd110de2c7ee317f48b2181e2255e943d6a7fa326","abstract_canon_sha256":"afa586619ad50b9e38e98500bf681316736d8ec81308f92207ebfad94de2b3d8"},"schema_version":"1.0"},"canonical_sha256":"72e56b0c8c57a6c4cbba1c5d5ab6202f73508767f15889ddc6c9302f5a79c413","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:02.986757Z","signature_b64":"wsy32dm2bm3Y4qSK69E4oBr30YDa1tioGGxXAdyPfFNMjDPWauJNtTtIQxEEoG0GVESP2/ULCvNXBoyGuB60Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72e56b0c8c57a6c4cbba1c5d5ab6202f73508767f15889ddc6c9302f5a79c413","last_reissued_at":"2026-05-18T03:23:02.986115Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:02.986115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.4250","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":"2026-05-18T03:23:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nVS1yP5/ewJ4+uM17dfqMx0PBFb04B8N1l9FMjQPqtz7x1BxKxFkjgNZJ6t+4rRbMNYwD61GWsCUj0Is1gPoDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T18:28:22.144276Z"},"content_sha256":"cc163351f0246b30e9a24052a8bd5b72477696f5f1836e3c5423cb4ad34ba70d","schema_version":"1.0","event_id":"sha256:cc163351f0246b30e9a24052a8bd5b72477696f5f1836e3c5423cb4ad34ba70d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:OLSWWDEMK6TMJS52DROVVNRAF5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Search for doubly-charged Higgs boson pair production in ppbar collisions at sqrt{s} = 1.96 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"D0 Collaboration","submitted_at":"2011-06-21T16:16:02Z","abstract_excerpt":"We present a search for pair production of doubly-charged Higgs bosons in the processes qqbar to H++H-- decaying through H++/-- to tau tau, muon tau, muon muon. The search is performed in ppbar collisions at a center-of-mass energy of sqrt{s}=1.96 TeV using an integrated luminosity of 7.0 fb-1 collected by the D0 experiment at the Fermilab Tevatron Collider. The results are used to set 95% C.L. limits on the pair production cross section of doubly-charged Higgs bosons and on their mass for different H++/-- branching fractions. Models predicting different H++/-- decays are investigated. Assumin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.4250","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":"2026-05-18T03:23:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ppTDBLx5vJwbFlGFieJABAndlc4NaPr9I98Ne6+TD0+R6H9hbvaGW1xfTSTlBrUPCIzrnajnToLsnxiHJfjwCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T18:28:22.144925Z"},"content_sha256":"14eac0dbcb7a363e7cd054da0cbf187878192518d3a05df4a2508c80948ef1d1","schema_version":"1.0","event_id":"sha256:14eac0dbcb7a363e7cd054da0cbf187878192518d3a05df4a2508c80948ef1d1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OLSWWDEMK6TMJS52DROVVNRAF5/bundle.json","state_url":"https://pith.science/pith/OLSWWDEMK6TMJS52DROVVNRAF5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OLSWWDEMK6TMJS52DROVVNRAF5/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":"2026-06-06T18:28:22Z","links":{"resolver":"https://pith.science/pith/OLSWWDEMK6TMJS52DROVVNRAF5","bundle":"https://pith.science/pith/OLSWWDEMK6TMJS52DROVVNRAF5/bundle.json","state":"https://pith.science/pith/OLSWWDEMK6TMJS52DROVVNRAF5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OLSWWDEMK6TMJS52DROVVNRAF5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:OLSWWDEMK6TMJS52DROVVNRAF5","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":"afa586619ad50b9e38e98500bf681316736d8ec81308f92207ebfad94de2b3d8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-06-21T16:16:02Z","title_canon_sha256":"7ad2bdb26cb58bb8a00d524fd110de2c7ee317f48b2181e2255e943d6a7fa326"},"schema_version":"1.0","source":{"id":"1106.4250","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.4250","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"arxiv_version","alias_value":"1106.4250v2","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.4250","created_at":"2026-05-18T03:23:02Z"},{"alias_kind":"pith_short_12","alias_value":"OLSWWDEMK6TM","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"OLSWWDEMK6TMJS52","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"OLSWWDEM","created_at":"2026-05-18T12:26:37Z"}],"graph_snapshots":[{"event_id":"sha256:14eac0dbcb7a363e7cd054da0cbf187878192518d3a05df4a2508c80948ef1d1","target":"graph","created_at":"2026-05-18T03:23:02Z","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 a search for pair production of doubly-charged Higgs bosons in the processes qqbar to H++H-- decaying through H++/-- to tau tau, muon tau, muon muon. The search is performed in ppbar collisions at a center-of-mass energy of sqrt{s}=1.96 TeV using an integrated luminosity of 7.0 fb-1 collected by the D0 experiment at the Fermilab Tevatron Collider. The results are used to set 95% C.L. limits on the pair production cross section of doubly-charged Higgs bosons and on their mass for different H++/-- branching fractions. Models predicting different H++/-- decays are investigated. Assumin","authors_text":"D0 Collaboration","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-06-21T16:16:02Z","title":"Search for doubly-charged Higgs boson pair production in ppbar collisions at sqrt{s} = 1.96 TeV"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.4250","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:cc163351f0246b30e9a24052a8bd5b72477696f5f1836e3c5423cb4ad34ba70d","target":"record","created_at":"2026-05-18T03:23:02Z","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":"afa586619ad50b9e38e98500bf681316736d8ec81308f92207ebfad94de2b3d8","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-06-21T16:16:02Z","title_canon_sha256":"7ad2bdb26cb58bb8a00d524fd110de2c7ee317f48b2181e2255e943d6a7fa326"},"schema_version":"1.0","source":{"id":"1106.4250","kind":"arxiv","version":2}},"canonical_sha256":"72e56b0c8c57a6c4cbba1c5d5ab6202f73508767f15889ddc6c9302f5a79c413","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"72e56b0c8c57a6c4cbba1c5d5ab6202f73508767f15889ddc6c9302f5a79c413","first_computed_at":"2026-05-18T03:23:02.986115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:23:02.986115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wsy32dm2bm3Y4qSK69E4oBr30YDa1tioGGxXAdyPfFNMjDPWauJNtTtIQxEEoG0GVESP2/ULCvNXBoyGuB60Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:23:02.986757Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.4250","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cc163351f0246b30e9a24052a8bd5b72477696f5f1836e3c5423cb4ad34ba70d","sha256:14eac0dbcb7a363e7cd054da0cbf187878192518d3a05df4a2508c80948ef1d1"],"state_sha256":"7cbcdf05c43455b2f0a03b7f3501f68a47233d5e079e4e1035be3b5013c2d2c6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4URq5Av8zQUkkW3mCrvnn1gDG/JKwv5QSZrmpLFaED7QeRvxffBPHoe6d2jv3ow+M8UoJ0ks/GtuoWYk4SbTAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T18:28:22.147424Z","bundle_sha256":"3b5a8ca5dbc0c0caf613eeecfd51cf0b7041e739ae33d6e2fe1a5200d1e08c7b"}}