{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:X6Q6PTLTCYSRNTHBH6V56RYOBG","short_pith_number":"pith:X6Q6PTLT","canonical_record":{"source":{"id":"hep-ph/0104179","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-04-18T15:17:03Z","cross_cats_sorted":[],"title_canon_sha256":"8a57fc94babd2759fb90d046f353f795bfd3eafd56c87ec4ffad0a8e047af0c5","abstract_canon_sha256":"bbe9544c4de44642ec7810182e5cde7e5c5a06e1064e30d739e46b17565f8ae2"},"schema_version":"1.0"},"canonical_sha256":"bfa1e7cd73162516cce13fabdf470e0996d0f0714d0ae54fdcc6109927c6e001","source":{"kind":"arxiv","id":"hep-ph/0104179","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0104179","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0104179v1","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0104179","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"pith_short_12","alias_value":"X6Q6PTLTCYSR","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"X6Q6PTLTCYSRNTHB","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"X6Q6PTLT","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:X6Q6PTLTCYSRNTHBH6V56RYOBG","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0104179","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-04-18T15:17:03Z","cross_cats_sorted":[],"title_canon_sha256":"8a57fc94babd2759fb90d046f353f795bfd3eafd56c87ec4ffad0a8e047af0c5","abstract_canon_sha256":"bbe9544c4de44642ec7810182e5cde7e5c5a06e1064e30d739e46b17565f8ae2"},"schema_version":"1.0"},"canonical_sha256":"bfa1e7cd73162516cce13fabdf470e0996d0f0714d0ae54fdcc6109927c6e001","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:14.918376Z","signature_b64":"P761LZLGoYOSymo7yVcfUdY2gVtlcND3/rzaHiA5VKyD9jXa9iXwlr337vLfhHr5gcVeEZljvZ1579nYvpHQBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bfa1e7cd73162516cce13fabdf470e0996d0f0714d0ae54fdcc6109927c6e001","last_reissued_at":"2026-05-18T01:06:14.917747Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:14.917747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0104179","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":"2026-05-18T01:06:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vQ74QLX00xZa9wfzoNPKHCsGZozqDk4VO7nq05BShDwLhUNsZS1bkaFG5fLGLSt3bM7aLY9bDfqBbEmNy1ZVBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:48:55.856227Z"},"content_sha256":"07a37a062dde061d09ae004d2a3a5637eb7c99b8f7be68ef66cc341efd204877","schema_version":"1.0","event_id":"sha256:07a37a062dde061d09ae004d2a3a5637eb7c99b8f7be68ef66cc341efd204877"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:X6Q6PTLTCYSRNTHBH6V56RYOBG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Can the charged Higgs boson be discovered in $e\\gamma$ collisions using the channel $e^-\\gamma\\to\\nu H^-$?","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kosuke Odagiri, Shinya Kanemura","submitted_at":"2001-04-18T15:17:03Z","abstract_excerpt":"We consider the single production of charged Higgs bosons $H^\\pm$ of the two-Higgs-doublet model in $e\\gamma$ collisions through the production subprocess $e^-\\gamma\\to\\nu H^-$.\n As the production rate is governed by the size of the loop-induced $H^\\pm W^\\mp\\gamma$ coupling, the cross section can only be substantial for smaller values of $\\tan\\beta$, $\\tan\\beta\\lesssim1$, where the top-bottom loop contribution is enhanced.\n In this case, however, the natural width of the charged Higgs boson becomes large so that the Standard Model continuum background becomes important. We study the background"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0104179","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":"2026-05-18T01:06:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2XLStXwATU+EWDf5HHXXy4NiO/3PXOqsOUCI5zooar+F5lOuN3l7iGrQ8j4hO5kNj+QKCtLxRN9/6VauDqvXDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:48:55.856611Z"},"content_sha256":"01f304e604362ca44af9d41777d4fb21dfd1a3f8333f9c13510b3b888d323623","schema_version":"1.0","event_id":"sha256:01f304e604362ca44af9d41777d4fb21dfd1a3f8333f9c13510b3b888d323623"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/bundle.json","state_url":"https://pith.science/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/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":"2026-06-01T13:48:55Z","links":{"resolver":"https://pith.science/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG","bundle":"https://pith.science/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/bundle.json","state":"https://pith.science/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/X6Q6PTLTCYSRNTHBH6V56RYOBG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:X6Q6PTLTCYSRNTHBH6V56RYOBG","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":"bbe9544c4de44642ec7810182e5cde7e5c5a06e1064e30d739e46b17565f8ae2","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-04-18T15:17:03Z","title_canon_sha256":"8a57fc94babd2759fb90d046f353f795bfd3eafd56c87ec4ffad0a8e047af0c5"},"schema_version":"1.0","source":{"id":"hep-ph/0104179","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0104179","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0104179v1","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0104179","created_at":"2026-05-18T01:06:14Z"},{"alias_kind":"pith_short_12","alias_value":"X6Q6PTLTCYSR","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"X6Q6PTLTCYSRNTHB","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"X6Q6PTLT","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:01f304e604362ca44af9d41777d4fb21dfd1a3f8333f9c13510b3b888d323623","target":"graph","created_at":"2026-05-18T01:06:14Z","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 consider the single production of charged Higgs bosons $H^\\pm$ of the two-Higgs-doublet model in $e\\gamma$ collisions through the production subprocess $e^-\\gamma\\to\\nu H^-$.\n As the production rate is governed by the size of the loop-induced $H^\\pm W^\\mp\\gamma$ coupling, the cross section can only be substantial for smaller values of $\\tan\\beta$, $\\tan\\beta\\lesssim1$, where the top-bottom loop contribution is enhanced.\n In this case, however, the natural width of the charged Higgs boson becomes large so that the Standard Model continuum background becomes important. We study the background","authors_text":"Kosuke Odagiri, Shinya Kanemura","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2001-04-18T15:17:03Z","title":"Can the charged Higgs boson be discovered in $e\\gamma$ collisions using the channel $e^-\\gamma\\to\\nu H^-$?"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0104179","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":"sha256:07a37a062dde061d09ae004d2a3a5637eb7c99b8f7be68ef66cc341efd204877","target":"record","created_at":"2026-05-18T01:06:14Z","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":"bbe9544c4de44642ec7810182e5cde7e5c5a06e1064e30d739e46b17565f8ae2","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-04-18T15:17:03Z","title_canon_sha256":"8a57fc94babd2759fb90d046f353f795bfd3eafd56c87ec4ffad0a8e047af0c5"},"schema_version":"1.0","source":{"id":"hep-ph/0104179","kind":"arxiv","version":1}},"canonical_sha256":"bfa1e7cd73162516cce13fabdf470e0996d0f0714d0ae54fdcc6109927c6e001","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bfa1e7cd73162516cce13fabdf470e0996d0f0714d0ae54fdcc6109927c6e001","first_computed_at":"2026-05-18T01:06:14.917747Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:14.917747Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"P761LZLGoYOSymo7yVcfUdY2gVtlcND3/rzaHiA5VKyD9jXa9iXwlr337vLfhHr5gcVeEZljvZ1579nYvpHQBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:14.918376Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0104179","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:07a37a062dde061d09ae004d2a3a5637eb7c99b8f7be68ef66cc341efd204877","sha256:01f304e604362ca44af9d41777d4fb21dfd1a3f8333f9c13510b3b888d323623"],"state_sha256":"07588e741a2eadc3796f3441623101e875a44a88571c6493a652ef221d238c3a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bqca8dWzQ9sTjqfL6Z0hlibYhMxEgXw8PmokKiBXa2jaUgmrc3ykgRKWVT6MJBsRrJmhRqFDDmtkNcU8tLhABQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:48:55.858818Z","bundle_sha256":"961ca9211e3e80960d32ffb4db01639c4d10a5f73809cf6c7c3593f79c2d289f"}}