{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:5WLUOTKVXB4LBC2Z7TBMKSKTKG","short_pith_number":"pith:5WLUOTKV","canonical_record":{"source":{"id":"hep-ph/0103050","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-05T15:57:19Z","cross_cats_sorted":[],"title_canon_sha256":"e5b3eb32efda61206fb72edd9be0830ae1aad31edbf6123c932351e2cc58fd55","abstract_canon_sha256":"4e3c5c304972324f8cb466d8c7d3de056e860e2db5539c99c76dc0dc500a942b"},"schema_version":"1.0"},"canonical_sha256":"ed97474d55b878b08b59fcc2c549535189a866bffccabc389359cf4791af33a4","source":{"kind":"arxiv","id":"hep-ph/0103050","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0103050","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0103050v1","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0103050","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"pith_short_12","alias_value":"5WLUOTKVXB4L","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"5WLUOTKVXB4LBC2Z","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"5WLUOTKV","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:5WLUOTKVXB4LBC2Z7TBMKSKTKG","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0103050","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-05T15:57:19Z","cross_cats_sorted":[],"title_canon_sha256":"e5b3eb32efda61206fb72edd9be0830ae1aad31edbf6123c932351e2cc58fd55","abstract_canon_sha256":"4e3c5c304972324f8cb466d8c7d3de056e860e2db5539c99c76dc0dc500a942b"},"schema_version":"1.0"},"canonical_sha256":"ed97474d55b878b08b59fcc2c549535189a866bffccabc389359cf4791af33a4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:31:38.665660Z","signature_b64":"mIS7ZXIysqsBqXzGMJbtKYlzqDWdEq0RpEfRbI2YrodBWCAAL5D0xpXogiNgNjRFrWTLrl/FwJNB9OZ7uth8AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed97474d55b878b08b59fcc2c549535189a866bffccabc389359cf4791af33a4","last_reissued_at":"2026-05-18T02:31:38.664971Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:31:38.664971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0103050","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":"2026-05-18T02:31:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s61uMIhUfQkcew31yhzMFngn62NFjbUz5d8QUjelSl72jV6A1p9rm2PO7YgsKIOJgFFgTrpbkSElMYS0yBvYDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T00:36:53.491268Z"},"content_sha256":"21e5ef343f3d231a7c04b4600c89190b25fd50bca5b315af22f35c415cb32cb8","schema_version":"1.0","event_id":"sha256:21e5ef343f3d231a7c04b4600c89190b25fd50bca5b315af22f35c415cb32cb8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:5WLUOTKVXB4LBC2Z7TBMKSKTKG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bounds for FCNC and the Pseudoscalar Higgs mass in the General Two Higgs Doublet Model type III using $g-2$ muon factor","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J.-Alexis Rodriguez, R. Martinez, Rodolfo A. Diaz","submitted_at":"2001-03-05T15:57:19Z","abstract_excerpt":"Current muon anomalous magnetic moment data have challenged the SM, and seems to open a window to new Physics. Since the difference between SM and experimental predictions is approximately $2.6\\sigma$. In the framework of the General Two Higgs Doublet Model (2HDM), we calculate the muon anomalous magnetic moment to get lower and upper bounds for the Flavor Changing Yukawa couplings (FC) in the leptonic sector. We also obtain lower bounds for the mass of the Pseudoscalar Higgs ($m_{A^ 0}$, as a function of the parameters of the model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0103050","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":"2026-05-18T02:31:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5z7XwDGgNXJOpS3vzRNinUWfY8UvIp5R3Zm34xUaigUh85d1je0nfnUup876GfY4lwBBlySLQbZKLiKwmjxsCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T00:36:53.491637Z"},"content_sha256":"e6c75df7f0111961e9986361213f226ab3325b8304ae59090f82233f952c0bdb","schema_version":"1.0","event_id":"sha256:e6c75df7f0111961e9986361213f226ab3325b8304ae59090f82233f952c0bdb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/bundle.json","state_url":"https://pith.science/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/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":"2026-06-29T00:36:53Z","links":{"resolver":"https://pith.science/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG","bundle":"https://pith.science/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/bundle.json","state":"https://pith.science/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5WLUOTKVXB4LBC2Z7TBMKSKTKG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:5WLUOTKVXB4LBC2Z7TBMKSKTKG","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":"4e3c5c304972324f8cb466d8c7d3de056e860e2db5539c99c76dc0dc500a942b","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-05T15:57:19Z","title_canon_sha256":"e5b3eb32efda61206fb72edd9be0830ae1aad31edbf6123c932351e2cc58fd55"},"schema_version":"1.0","source":{"id":"hep-ph/0103050","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0103050","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0103050v1","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0103050","created_at":"2026-05-18T02:31:38Z"},{"alias_kind":"pith_short_12","alias_value":"5WLUOTKVXB4L","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"5WLUOTKVXB4LBC2Z","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"5WLUOTKV","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:e6c75df7f0111961e9986361213f226ab3325b8304ae59090f82233f952c0bdb","target":"graph","created_at":"2026-05-18T02:31:38Z","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":"Current muon anomalous magnetic moment data have challenged the SM, and seems to open a window to new Physics. Since the difference between SM and experimental predictions is approximately $2.6\\sigma$. In the framework of the General Two Higgs Doublet Model (2HDM), we calculate the muon anomalous magnetic moment to get lower and upper bounds for the Flavor Changing Yukawa couplings (FC) in the leptonic sector. We also obtain lower bounds for the mass of the Pseudoscalar Higgs ($m_{A^ 0}$, as a function of the parameters of the model.","authors_text":"J.-Alexis Rodriguez, R. Martinez, Rodolfo A. Diaz","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2001-03-05T15:57:19Z","title":"Bounds for FCNC and the Pseudoscalar Higgs mass in the General Two Higgs Doublet Model type III using $g-2$ muon factor"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0103050","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":"sha256:21e5ef343f3d231a7c04b4600c89190b25fd50bca5b315af22f35c415cb32cb8","target":"record","created_at":"2026-05-18T02:31:38Z","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":"4e3c5c304972324f8cb466d8c7d3de056e860e2db5539c99c76dc0dc500a942b","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-05T15:57:19Z","title_canon_sha256":"e5b3eb32efda61206fb72edd9be0830ae1aad31edbf6123c932351e2cc58fd55"},"schema_version":"1.0","source":{"id":"hep-ph/0103050","kind":"arxiv","version":1}},"canonical_sha256":"ed97474d55b878b08b59fcc2c549535189a866bffccabc389359cf4791af33a4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ed97474d55b878b08b59fcc2c549535189a866bffccabc389359cf4791af33a4","first_computed_at":"2026-05-18T02:31:38.664971Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:31:38.664971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mIS7ZXIysqsBqXzGMJbtKYlzqDWdEq0RpEfRbI2YrodBWCAAL5D0xpXogiNgNjRFrWTLrl/FwJNB9OZ7uth8AA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:31:38.665660Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0103050","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:21e5ef343f3d231a7c04b4600c89190b25fd50bca5b315af22f35c415cb32cb8","sha256:e6c75df7f0111961e9986361213f226ab3325b8304ae59090f82233f952c0bdb"],"state_sha256":"c0119b68247c1baa44482261b5d9b44c031772ea7ed557fee084538fe5395a39"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+U6PtZgwbAYpa+JTHvhFal6s/KrRwVQ9WryKEZRADCxsU5dZ13V2f40ibKpZ9/u2/x3A2qOGCYiN3zFeDKuqAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T00:36:53.493623Z","bundle_sha256":"cc05d1c064d7635a6427da10fc42ae92f7714cdf3373aa69533d95375f76f502"}}