{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:UMVNPKL6ENTYXULQ4INA6ZDHKN","short_pith_number":"pith:UMVNPKL6","canonical_record":{"source":{"id":"1903.04560","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-03-11T19:40:49Z","cross_cats_sorted":[],"title_canon_sha256":"3416831fe67231deab10d6477cd3e1f6fb0c5c2b07f18999499ad4d7a380d33a","abstract_canon_sha256":"33ac6f35f0eecc5af41e8257473716aad43f1189dc87789cbfda812ac6862452"},"schema_version":"1.0"},"canonical_sha256":"a32ad7a97e23678bd170e21a0f6467536e21e78308258a1098627eb800711768","source":{"kind":"arxiv","id":"1903.04560","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1903.04560","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"arxiv_version","alias_value":"1903.04560v2","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.04560","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"pith_short_12","alias_value":"UMVNPKL6ENTY","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_16","alias_value":"UMVNPKL6ENTYXULQ","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_8","alias_value":"UMVNPKL6","created_at":"2026-05-18T12:33:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:UMVNPKL6ENTYXULQ4INA6ZDHKN","target":"record","payload":{"canonical_record":{"source":{"id":"1903.04560","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-03-11T19:40:49Z","cross_cats_sorted":[],"title_canon_sha256":"3416831fe67231deab10d6477cd3e1f6fb0c5c2b07f18999499ad4d7a380d33a","abstract_canon_sha256":"33ac6f35f0eecc5af41e8257473716aad43f1189dc87789cbfda812ac6862452"},"schema_version":"1.0"},"canonical_sha256":"a32ad7a97e23678bd170e21a0f6467536e21e78308258a1098627eb800711768","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:24.676554Z","signature_b64":"l1ljXq+pd/fTHX/fd2R/VFl32LTGi6ooFc5aCkCgsnO8WSoROBkLsj+LYyR+lT7KzZrmMyc+7BTgfIrKS3jNBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a32ad7a97e23678bd170e21a0f6467536e21e78308258a1098627eb800711768","last_reissued_at":"2026-05-17T23:39:24.675926Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:24.675926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1903.04560","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":"2026-05-17T23:39:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zFNF2C5IdEaepOEy1M4noayXtPkqsizpLXeHXqIaiWI2RUy4oGxliTRDQ/TSZHJWPpl0xeCdvqmj7rtFjMgCDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:34:34.234218Z"},"content_sha256":"088e6f617ac4e46cde5c5460fe29b34d561a5d75c3d95e9df5a6369c4c3c7e6a","schema_version":"1.0","event_id":"sha256:088e6f617ac4e46cde5c5460fe29b34d561a5d75c3d95e9df5a6369c4c3c7e6a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:UMVNPKL6ENTYXULQ4INA6ZDHKN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Search for charged Higgs bosons in the H$^{\\pm}$ $\\to$ $\\tau^{\\pm}\\nu_\\tau$ decay channel in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2019-03-11T19:40:49Z","abstract_excerpt":"A search is presented for charged Higgs bosons in the H$^{\\pm}$ $\\to$ $\\tau^{\\pm}\\nu_\\tau$ decay mode in the hadronic final state and in final states with an electron or muon. The search is based on proton-proton collision data recorded by the CMS experiment in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. The results agree with the background expectation from the standard model. Upper limits at 95% confidence level are set on the production cross section times branching fraction to $\\tau^{\\pm}\\nu_\\tau$ for an H$^{\\pm}$ in the mass rang"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.04560","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":"2026-05-17T23:39:24Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nhi+sXdBK0/cdRMLfhGnHqIMX6m7lj7jWW57Y48WU/GmBID447rIrbPGykXAu5frX86HQHLXjEyEQN4dekm0Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:34:34.234580Z"},"content_sha256":"223046e546981e94d48d346c42a1c22ef61e91074cfe80c94bf6607a323c85ea","schema_version":"1.0","event_id":"sha256:223046e546981e94d48d346c42a1c22ef61e91074cfe80c94bf6607a323c85ea"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/bundle.json","state_url":"https://pith.science/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/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":"2026-05-28T01:34:34Z","links":{"resolver":"https://pith.science/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN","bundle":"https://pith.science/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/bundle.json","state":"https://pith.science/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UMVNPKL6ENTYXULQ4INA6ZDHKN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:UMVNPKL6ENTYXULQ4INA6ZDHKN","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":"33ac6f35f0eecc5af41e8257473716aad43f1189dc87789cbfda812ac6862452","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-03-11T19:40:49Z","title_canon_sha256":"3416831fe67231deab10d6477cd3e1f6fb0c5c2b07f18999499ad4d7a380d33a"},"schema_version":"1.0","source":{"id":"1903.04560","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1903.04560","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"arxiv_version","alias_value":"1903.04560v2","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.04560","created_at":"2026-05-17T23:39:24Z"},{"alias_kind":"pith_short_12","alias_value":"UMVNPKL6ENTY","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_16","alias_value":"UMVNPKL6ENTYXULQ","created_at":"2026-05-18T12:33:30Z"},{"alias_kind":"pith_short_8","alias_value":"UMVNPKL6","created_at":"2026-05-18T12:33:30Z"}],"graph_snapshots":[{"event_id":"sha256:223046e546981e94d48d346c42a1c22ef61e91074cfe80c94bf6607a323c85ea","target":"graph","created_at":"2026-05-17T23:39:24Z","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":"A search is presented for charged Higgs bosons in the H$^{\\pm}$ $\\to$ $\\tau^{\\pm}\\nu_\\tau$ decay mode in the hadronic final state and in final states with an electron or muon. The search is based on proton-proton collision data recorded by the CMS experiment in 2016 at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. The results agree with the background expectation from the standard model. Upper limits at 95% confidence level are set on the production cross section times branching fraction to $\\tau^{\\pm}\\nu_\\tau$ for an H$^{\\pm}$ in the mass rang","authors_text":"CMS Collaboration","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-03-11T19:40:49Z","title":"Search for charged Higgs bosons in the H$^{\\pm}$ $\\to$ $\\tau^{\\pm}\\nu_\\tau$ decay channel in proton-proton collisions at $\\sqrt{s} =$ 13 TeV"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.04560","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":"sha256:088e6f617ac4e46cde5c5460fe29b34d561a5d75c3d95e9df5a6369c4c3c7e6a","target":"record","created_at":"2026-05-17T23:39:24Z","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":"33ac6f35f0eecc5af41e8257473716aad43f1189dc87789cbfda812ac6862452","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-03-11T19:40:49Z","title_canon_sha256":"3416831fe67231deab10d6477cd3e1f6fb0c5c2b07f18999499ad4d7a380d33a"},"schema_version":"1.0","source":{"id":"1903.04560","kind":"arxiv","version":2}},"canonical_sha256":"a32ad7a97e23678bd170e21a0f6467536e21e78308258a1098627eb800711768","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a32ad7a97e23678bd170e21a0f6467536e21e78308258a1098627eb800711768","first_computed_at":"2026-05-17T23:39:24.675926Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:39:24.675926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"l1ljXq+pd/fTHX/fd2R/VFl32LTGi6ooFc5aCkCgsnO8WSoROBkLsj+LYyR+lT7KzZrmMyc+7BTgfIrKS3jNBw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:39:24.676554Z","signed_message":"canonical_sha256_bytes"},"source_id":"1903.04560","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:088e6f617ac4e46cde5c5460fe29b34d561a5d75c3d95e9df5a6369c4c3c7e6a","sha256:223046e546981e94d48d346c42a1c22ef61e91074cfe80c94bf6607a323c85ea"],"state_sha256":"abf070009905dd4e641a47ac25bc0ed92c84df5225fb85e17d5a45eca1dc5257"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1Eh28Za2uIyRpIyBH44UcK6aaI84Hatgnx+xR8krBJ1EKkWaV6Nz3Vqjdw2yJALbseUSzEz+TOPvVt2tFJbXCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T01:34:34.236631Z","bundle_sha256":"bf97390226075f6757fec9fd36d43f200728035395fad1833bb91162f65b35c9"}}