{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:BXYJQF77S2WLXHNCBMS2E7ANHX","short_pith_number":"pith:BXYJQF77","canonical_record":{"source":{"id":"hep-ph/0410374","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-10-27T22:18:26Z","cross_cats_sorted":[],"title_canon_sha256":"1b6ac2249f01072a2c0bfd158d8b2bc54c6568e9312350600baaf68cc0f8ae4f","abstract_canon_sha256":"a49771f41821cf82c556f123339dcb079b3f5e3540ce90bfecb0428e79c00e4d"},"schema_version":"1.0"},"canonical_sha256":"0df09817ff96acbb9da20b25a27c0d3dd2029afd43e9cb4e22e4bc178d98c594","source":{"kind":"arxiv","id":"hep-ph/0410374","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0410374","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0410374v1","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0410374","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"pith_short_12","alias_value":"BXYJQF77S2WL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"BXYJQF77S2WLXHNC","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"BXYJQF77","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:BXYJQF77S2WLXHNCBMS2E7ANHX","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0410374","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-10-27T22:18:26Z","cross_cats_sorted":[],"title_canon_sha256":"1b6ac2249f01072a2c0bfd158d8b2bc54c6568e9312350600baaf68cc0f8ae4f","abstract_canon_sha256":"a49771f41821cf82c556f123339dcb079b3f5e3540ce90bfecb0428e79c00e4d"},"schema_version":"1.0"},"canonical_sha256":"0df09817ff96acbb9da20b25a27c0d3dd2029afd43e9cb4e22e4bc178d98c594","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:05.390367Z","signature_b64":"TQ6BCxPISpPSXcXLnq09z5dp/fMxJOT4d2Mz8HQeOyA4D9O3A3JRNdbul57um4w6RmanpasOrFhiaCaFNUywDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0df09817ff96acbb9da20b25a27c0d3dd2029afd43e9cb4e22e4bc178d98c594","last_reissued_at":"2026-05-18T01:39:05.389716Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:05.389716Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0410374","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":"2026-05-18T01:39:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O5TOmt4XUH4MqP4594/fFBStNlHA5BxY96TMgDxcVlNkDsAfuhqm0IeoJ6ZNwAD1PoeEDqmTP/d9POfPdyz7Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T00:26:10.547055Z"},"content_sha256":"0e86cdb20fac0c49927b7e94bcfd6f9e68464c303c3c7f5c286050d58628802f","schema_version":"1.0","event_id":"sha256:0e86cdb20fac0c49927b7e94bcfd6f9e68464c303c3c7f5c286050d58628802f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:BXYJQF77S2WLXHNCBMS2E7ANHX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effective Lagrangian for Charged Higgs Couplings","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anastasios Psinas, Tarek Ibrahim","submitted_at":"2004-10-27T22:18:26Z","abstract_excerpt":"The effective Lagrangian including one loop corrections is deduced for the couplings of the charged Higgs with quarks and leptons, and with charginos and neutralinos. The effect of the one loop corrections is found to be quite significant in a number of sectors. The effective Lagrangian is then used to analyze the decay of the charged Higgs into a number of decay channels. Specifically we consider the decay of $H^+(H^-)$ into the decay modes $t\\bar b$ ($\\bar t b$), $\\bar\\tau\\nu_{\\tau}$ ($\\tau \\bar \\nu_{\\tau}$), and $\\chi_i^+\\chi_j^0(\\chi_i^-\\chi_j^0)$ (i=1,2; j=1-4). The loop corrections to th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0410374","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":"2026-05-18T01:39:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OCiNFFSIq6SrpSHTKdZQTCU+vLFi1JEHP5N3xuAR3zSsFTAsOMJG/BFDHCO+LMXW4cJzUXutkw+etxSb2MJKDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T00:26:10.547407Z"},"content_sha256":"354d055417d6653e00db95f92fc9ff429d62e3c7cf2a7acf92c92f4238c84b6f","schema_version":"1.0","event_id":"sha256:354d055417d6653e00db95f92fc9ff429d62e3c7cf2a7acf92c92f4238c84b6f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/bundle.json","state_url":"https://pith.science/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/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":"2026-07-05T00:26:10Z","links":{"resolver":"https://pith.science/pith/BXYJQF77S2WLXHNCBMS2E7ANHX","bundle":"https://pith.science/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/bundle.json","state":"https://pith.science/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BXYJQF77S2WLXHNCBMS2E7ANHX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:BXYJQF77S2WLXHNCBMS2E7ANHX","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":"a49771f41821cf82c556f123339dcb079b3f5e3540ce90bfecb0428e79c00e4d","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-10-27T22:18:26Z","title_canon_sha256":"1b6ac2249f01072a2c0bfd158d8b2bc54c6568e9312350600baaf68cc0f8ae4f"},"schema_version":"1.0","source":{"id":"hep-ph/0410374","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0410374","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0410374v1","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0410374","created_at":"2026-05-18T01:39:05Z"},{"alias_kind":"pith_short_12","alias_value":"BXYJQF77S2WL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"BXYJQF77S2WLXHNC","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"BXYJQF77","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:354d055417d6653e00db95f92fc9ff429d62e3c7cf2a7acf92c92f4238c84b6f","target":"graph","created_at":"2026-05-18T01:39:05Z","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":"The effective Lagrangian including one loop corrections is deduced for the couplings of the charged Higgs with quarks and leptons, and with charginos and neutralinos. The effect of the one loop corrections is found to be quite significant in a number of sectors. The effective Lagrangian is then used to analyze the decay of the charged Higgs into a number of decay channels. Specifically we consider the decay of $H^+(H^-)$ into the decay modes $t\\bar b$ ($\\bar t b$), $\\bar\\tau\\nu_{\\tau}$ ($\\tau \\bar \\nu_{\\tau}$), and $\\chi_i^+\\chi_j^0(\\chi_i^-\\chi_j^0)$ (i=1,2; j=1-4). The loop corrections to th","authors_text":"Anastasios Psinas, Tarek Ibrahim","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2004-10-27T22:18:26Z","title":"Effective Lagrangian for Charged Higgs Couplings"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0410374","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":"sha256:0e86cdb20fac0c49927b7e94bcfd6f9e68464c303c3c7f5c286050d58628802f","target":"record","created_at":"2026-05-18T01:39:05Z","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":"a49771f41821cf82c556f123339dcb079b3f5e3540ce90bfecb0428e79c00e4d","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2004-10-27T22:18:26Z","title_canon_sha256":"1b6ac2249f01072a2c0bfd158d8b2bc54c6568e9312350600baaf68cc0f8ae4f"},"schema_version":"1.0","source":{"id":"hep-ph/0410374","kind":"arxiv","version":1}},"canonical_sha256":"0df09817ff96acbb9da20b25a27c0d3dd2029afd43e9cb4e22e4bc178d98c594","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0df09817ff96acbb9da20b25a27c0d3dd2029afd43e9cb4e22e4bc178d98c594","first_computed_at":"2026-05-18T01:39:05.389716Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:05.389716Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TQ6BCxPISpPSXcXLnq09z5dp/fMxJOT4d2Mz8HQeOyA4D9O3A3JRNdbul57um4w6RmanpasOrFhiaCaFNUywDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:05.390367Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0410374","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0e86cdb20fac0c49927b7e94bcfd6f9e68464c303c3c7f5c286050d58628802f","sha256:354d055417d6653e00db95f92fc9ff429d62e3c7cf2a7acf92c92f4238c84b6f"],"state_sha256":"a315b1395cebc0f1031c51808bc346b4325dafab0991a0cbe986346aa4cdb6b0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"91/RJ4TA8c3+wRo5Q2I5RgjappNGPZ0DX71aQFb7SCS/KgsALY3z81UqbkUbrjOT/WPjMfu5PDGN9T6wibElCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T00:26:10.549190Z","bundle_sha256":"804c703d6e3e0b85a10b7b6135e3000cc75e9aca806e5dda162bbb038fda096b"}}