{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:XCSJGLWK25SIMZ7KAQ5WKD5X2E","short_pith_number":"pith:XCSJGLWK","canonical_record":{"source":{"id":"1303.0983","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c5bac9cf0bd141117c57aa943dcc6ea596530cf150e86d4d3eac57b0110faa52","abstract_canon_sha256":"99c3f2fb165d52695ee28c2e00b76785f8fe3a8675eeb7268411c7a063f34883"},"schema_version":"1.0"},"canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","source":{"kind":"arxiv","id":"1303.0983","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.0983","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"arxiv_version","alias_value":"1303.0983v1","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0983","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"pith_short_12","alias_value":"XCSJGLWK25SI","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"XCSJGLWK25SIMZ7K","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"XCSJGLWK","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:XCSJGLWK25SIMZ7KAQ5WKD5X2E","target":"record","payload":{"canonical_record":{"source":{"id":"1303.0983","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"c5bac9cf0bd141117c57aa943dcc6ea596530cf150e86d4d3eac57b0110faa52","abstract_canon_sha256":"99c3f2fb165d52695ee28c2e00b76785f8fe3a8675eeb7268411c7a063f34883"},"schema_version":"1.0"},"canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:53.263087Z","signature_b64":"CyBGpg2erCtJfpPSZSyFiQwplS7S6zAxsMkluSQsv2Gihu7j8VhpD7itss4hB5oPqR689RPHB1OZXsSiaPdvAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","last_reissued_at":"2026-05-18T03:31:53.262503Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:53.262503Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.0983","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":"2026-05-18T03:31:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uUQwiYQMz9cL4mTa5Nsf1bqXrmnUcqDcEgWgYLJIwEzAZMKGB6y6vB2ie34aAvqPPcyR8kajvgAwcHQJ6eCiAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:44:01.242220Z"},"content_sha256":"40501cec82dde4703270dab6c4d4120254554cbb32feeefe7d27e50b1855bc58","schema_version":"1.0","event_id":"sha256:40501cec82dde4703270dab6c4d4120254554cbb32feeefe7d27e50b1855bc58"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:XCSJGLWK25SIMZ7KAQ5WKD5X2E","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charged Higgs boson production in single top mode at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Renato Guedes, Rui Santos, Stefano Moretti","submitted_at":"2013-03-05T11:08:28Z","abstract_excerpt":"The main production mode for a light charged Higgs boson at the LHC is $pp \\to t \\bar t$, with one the top-quarks decaying to a charged Higgs and a $b$-quark. However, single top production also gives rise to final states with charged Higgs bosons. In this work we analyse how the two processes compare at the LHC@14TeV. We will be working in the framework of the two-Higgs double model, considering both a CP-conserving and a CP-violating version of the model. We conclude that the single top mode could help to constrain the parameter space in several versions of the model. We also discuss the rol"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0983","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":"2026-05-18T03:31:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z2rUjVe+/+K+1OERnj0G8n23FzVtQfm0A5D4Elff36IHlCbzn914IdW91rt+CU8leWBTOJWwIyOVpK0cggzCBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T20:44:01.242892Z"},"content_sha256":"41b014b80ed2735143826c435f7e8b0388d40c1cc8484ae8b7d76a12eaba041d","schema_version":"1.0","event_id":"sha256:41b014b80ed2735143826c435f7e8b0388d40c1cc8484ae8b7d76a12eaba041d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/bundle.json","state_url":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/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":"2026-05-28T20:44:01Z","links":{"resolver":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E","bundle":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/bundle.json","state":"https://pith.science/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XCSJGLWK25SIMZ7KAQ5WKD5X2E/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:XCSJGLWK25SIMZ7KAQ5WKD5X2E","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":"99c3f2fb165d52695ee28c2e00b76785f8fe3a8675eeb7268411c7a063f34883","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","title_canon_sha256":"c5bac9cf0bd141117c57aa943dcc6ea596530cf150e86d4d3eac57b0110faa52"},"schema_version":"1.0","source":{"id":"1303.0983","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.0983","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"arxiv_version","alias_value":"1303.0983v1","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0983","created_at":"2026-05-18T03:31:53Z"},{"alias_kind":"pith_short_12","alias_value":"XCSJGLWK25SI","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"XCSJGLWK25SIMZ7K","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"XCSJGLWK","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:41b014b80ed2735143826c435f7e8b0388d40c1cc8484ae8b7d76a12eaba041d","target":"graph","created_at":"2026-05-18T03:31:53Z","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 main production mode for a light charged Higgs boson at the LHC is $pp \\to t \\bar t$, with one the top-quarks decaying to a charged Higgs and a $b$-quark. However, single top production also gives rise to final states with charged Higgs bosons. In this work we analyse how the two processes compare at the LHC@14TeV. We will be working in the framework of the two-Higgs double model, considering both a CP-conserving and a CP-violating version of the model. We conclude that the single top mode could help to constrain the parameter space in several versions of the model. We also discuss the rol","authors_text":"Renato Guedes, Rui Santos, Stefano Moretti","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","title":"Charged Higgs boson production in single top mode at the LHC"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0983","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":"sha256:40501cec82dde4703270dab6c4d4120254554cbb32feeefe7d27e50b1855bc58","target":"record","created_at":"2026-05-18T03:31:53Z","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":"99c3f2fb165d52695ee28c2e00b76785f8fe3a8675eeb7268411c7a063f34883","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-05T11:08:28Z","title_canon_sha256":"c5bac9cf0bd141117c57aa943dcc6ea596530cf150e86d4d3eac57b0110faa52"},"schema_version":"1.0","source":{"id":"1303.0983","kind":"arxiv","version":1}},"canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b8a4932ecad7648667ea043b650fb7d13bd2de8f5225347ff34a1e4e63bb5406","first_computed_at":"2026-05-18T03:31:53.262503Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:31:53.262503Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CyBGpg2erCtJfpPSZSyFiQwplS7S6zAxsMkluSQsv2Gihu7j8VhpD7itss4hB5oPqR689RPHB1OZXsSiaPdvAg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:31:53.263087Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.0983","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:40501cec82dde4703270dab6c4d4120254554cbb32feeefe7d27e50b1855bc58","sha256:41b014b80ed2735143826c435f7e8b0388d40c1cc8484ae8b7d76a12eaba041d"],"state_sha256":"521612ba2f65b71a19992b8db41f4301d827275bc1bfcd111d9db63d179f2f07"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lNC9AMQbRVLoouHzl9kYiilDdp2UjZ5UtDLEOHhpukI8ktGqTQAdTDpzxPnt3nKyQAf8hUmLe8JIAWwDA3foAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T20:44:01.245937Z","bundle_sha256":"108e2f9e06a968973eafb6855e77184da76a6efbdf43a75cd22207a2882d5bbd"}}