{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:2KEL7ZIXFGABBF7WMOEC5A4B5M","short_pith_number":"pith:2KEL7ZIX","canonical_record":{"source":{"id":"1401.4841","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-20T09:44:45Z","cross_cats_sorted":[],"title_canon_sha256":"dac6c2fdfb0cd8c0d39ec76bec018e64de2765cfe1facc939f16639c9c1f0f3a","abstract_canon_sha256":"fdba1bb8ba1371482bee2a819fccb7ccadea3823d027c5273291ac742b311884"},"schema_version":"1.0"},"canonical_sha256":"d288bfe51729801097f663882e8381eb34c2ab79a62f55fec25decb0d0152ca6","source":{"kind":"arxiv","id":"1401.4841","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.4841","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"arxiv_version","alias_value":"1401.4841v4","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.4841","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"pith_short_12","alias_value":"2KEL7ZIXFGAB","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2KEL7ZIXFGABBF7W","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2KEL7ZIX","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:2KEL7ZIXFGABBF7WMOEC5A4B5M","target":"record","payload":{"canonical_record":{"source":{"id":"1401.4841","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-20T09:44:45Z","cross_cats_sorted":[],"title_canon_sha256":"dac6c2fdfb0cd8c0d39ec76bec018e64de2765cfe1facc939f16639c9c1f0f3a","abstract_canon_sha256":"fdba1bb8ba1371482bee2a819fccb7ccadea3823d027c5273291ac742b311884"},"schema_version":"1.0"},"canonical_sha256":"d288bfe51729801097f663882e8381eb34c2ab79a62f55fec25decb0d0152ca6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:58.786742Z","signature_b64":"GBq8phjLpJM2PoE2P6SjmiwWHonmbuu5b8+yQIGnfraJhVMg4QuBFOQDaXVYhOmerybIJ2mqzpFP9F4sXSGQCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d288bfe51729801097f663882e8381eb34c2ab79a62f55fec25decb0d0152ca6","last_reissued_at":"2026-05-18T01:41:58.786251Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:58.786251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1401.4841","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:41:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"11cakNIdPdKB3yCeZVlhFLgRTYRMjrJ0pPanBKwYKE+OZo1g1Rm3B2xfMvyPFSgKMfs8Cmv10yoplpMceXAgCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:54:12.051533Z"},"content_sha256":"f5e6bec4cb29caff458041ab8e4802d7883c02890396120230170d566f8adca5","schema_version":"1.0","event_id":"sha256:f5e6bec4cb29caff458041ab8e4802d7883c02890396120230170d566f8adca5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:2KEL7ZIXFGABBF7WMOEC5A4B5M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Observability of Charged Higgs through Triple or Double Higgs Production in a General Two Higgs Doublet Model at an e+e- Linear Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ijaz Ahmed, Majid Hashemi","submitted_at":"2014-01-20T09:44:45Z","abstract_excerpt":"In this paper the triple Higgs production in a general two Higgs doublet model (2HDM) is studied. The production process is e+e- -> H+H-H0 followed by the charged Higgs decay to a pair of tau nu and the neutral Higgs decay to bb. The alternative process H+W-H0 is also included as a source of charged Higgs signal in the analysis. The focus is on a future e+e- linear collider operating at sqrt(s) = 1.5 TeV. The final state under consideration (tau tau bb ETmiss) is suitable for electroweak background rejection using the b-tagging tools. It is shown that although the signal cross section is small"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.4841","kind":"arxiv","version":4},"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":"2026-05-18T01:41:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w1I432dJCpHz0mohb6peRFWd2utxEX625TC3p7fsAHNwf1j3KpC9IHjVJUFONs2gnc0GP0TEDla/lDqeHW3QBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:54:12.052198Z"},"content_sha256":"c2f097f00e5de137ca68b4ac9b1ab87ee87e40abf44ed56db668cde92555f6bb","schema_version":"1.0","event_id":"sha256:c2f097f00e5de137ca68b4ac9b1ab87ee87e40abf44ed56db668cde92555f6bb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/bundle.json","state_url":"https://pith.science/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/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":"2026-05-30T06:54:12Z","links":{"resolver":"https://pith.science/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M","bundle":"https://pith.science/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/bundle.json","state":"https://pith.science/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2KEL7ZIXFGABBF7WMOEC5A4B5M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2KEL7ZIXFGABBF7WMOEC5A4B5M","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":"fdba1bb8ba1371482bee2a819fccb7ccadea3823d027c5273291ac742b311884","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-20T09:44:45Z","title_canon_sha256":"dac6c2fdfb0cd8c0d39ec76bec018e64de2765cfe1facc939f16639c9c1f0f3a"},"schema_version":"1.0","source":{"id":"1401.4841","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1401.4841","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"arxiv_version","alias_value":"1401.4841v4","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1401.4841","created_at":"2026-05-18T01:41:58Z"},{"alias_kind":"pith_short_12","alias_value":"2KEL7ZIXFGAB","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2KEL7ZIXFGABBF7W","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2KEL7ZIX","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:c2f097f00e5de137ca68b4ac9b1ab87ee87e40abf44ed56db668cde92555f6bb","target":"graph","created_at":"2026-05-18T01:41:58Z","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":"In this paper the triple Higgs production in a general two Higgs doublet model (2HDM) is studied. The production process is e+e- -> H+H-H0 followed by the charged Higgs decay to a pair of tau nu and the neutral Higgs decay to bb. The alternative process H+W-H0 is also included as a source of charged Higgs signal in the analysis. The focus is on a future e+e- linear collider operating at sqrt(s) = 1.5 TeV. The final state under consideration (tau tau bb ETmiss) is suitable for electroweak background rejection using the b-tagging tools. It is shown that although the signal cross section is small","authors_text":"Ijaz Ahmed, Majid Hashemi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-20T09:44:45Z","title":"Observability of Charged Higgs through Triple or Double Higgs Production in a General Two Higgs Doublet Model at an e+e- Linear Collider"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1401.4841","kind":"arxiv","version":4},"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:f5e6bec4cb29caff458041ab8e4802d7883c02890396120230170d566f8adca5","target":"record","created_at":"2026-05-18T01:41:58Z","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":"fdba1bb8ba1371482bee2a819fccb7ccadea3823d027c5273291ac742b311884","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-01-20T09:44:45Z","title_canon_sha256":"dac6c2fdfb0cd8c0d39ec76bec018e64de2765cfe1facc939f16639c9c1f0f3a"},"schema_version":"1.0","source":{"id":"1401.4841","kind":"arxiv","version":4}},"canonical_sha256":"d288bfe51729801097f663882e8381eb34c2ab79a62f55fec25decb0d0152ca6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d288bfe51729801097f663882e8381eb34c2ab79a62f55fec25decb0d0152ca6","first_computed_at":"2026-05-18T01:41:58.786251Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:58.786251Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GBq8phjLpJM2PoE2P6SjmiwWHonmbuu5b8+yQIGnfraJhVMg4QuBFOQDaXVYhOmerybIJ2mqzpFP9F4sXSGQCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:58.786742Z","signed_message":"canonical_sha256_bytes"},"source_id":"1401.4841","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f5e6bec4cb29caff458041ab8e4802d7883c02890396120230170d566f8adca5","sha256:c2f097f00e5de137ca68b4ac9b1ab87ee87e40abf44ed56db668cde92555f6bb"],"state_sha256":"c8a5dfd217777d35a806b36cef7c27c6b10faafe405f67444845caf9ad4dcdc5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xeEU+qnPu+rfQrBGCLUY+mBsgkeTbT1OTOanGlJ8c6Ytt1kLtAJuOjO81FvJMk/eFOL5XBFTt+3e8DRHO54JCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:54:12.055165Z","bundle_sha256":"10422b4e9fab6767218e0e7c5aa350873ec5c506ffbb564253bbce3f9541fb24"}}