{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:TBICBQSV75HBHFRP3Z3J6J3JNP","short_pith_number":"pith:TBICBQSV","canonical_record":{"source":{"id":"1603.01208","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-03T18:15:58Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e0321b5ef5654be2954aca761a30ff4befbedb5d15f0a0b07040b977c0608e44","abstract_canon_sha256":"5ea28fec8e5eb616e62a760a007b0737b431f07fcb7f2d8f440eed54e55424be"},"schema_version":"1.0"},"canonical_sha256":"985020c255ff4e13962fde769f27696bf8ff411cd9edf14f013aee55ef8b739d","source":{"kind":"arxiv","id":"1603.01208","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.01208","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"arxiv_version","alias_value":"1603.01208v2","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01208","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"pith_short_12","alias_value":"TBICBQSV75HB","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"TBICBQSV75HBHFRP","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"TBICBQSV","created_at":"2026-05-18T12:30:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:TBICBQSV75HBHFRP3Z3J6J3JNP","target":"record","payload":{"canonical_record":{"source":{"id":"1603.01208","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-03T18:15:58Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"e0321b5ef5654be2954aca761a30ff4befbedb5d15f0a0b07040b977c0608e44","abstract_canon_sha256":"5ea28fec8e5eb616e62a760a007b0737b431f07fcb7f2d8f440eed54e55424be"},"schema_version":"1.0"},"canonical_sha256":"985020c255ff4e13962fde769f27696bf8ff411cd9edf14f013aee55ef8b739d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:15.348437Z","signature_b64":"Sz7NxZfRKRKQHjPE49LKn19PY63aCMvm+eefkaEgWZfvKdE4vf85UuwBtVChM+WSwDIqtHJAh54cBWWM1ahoBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"985020c255ff4e13962fde769f27696bf8ff411cd9edf14f013aee55ef8b739d","last_reissued_at":"2026-05-18T00:47:15.347729Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:15.347729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1603.01208","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:47:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Y944gxE9BUf870PDygCG1fPgocDa5IyDxwVDgZnkGa90pJxF2crV58kwUD9I3rvyKHoO+xSwvCq37hpPiKqjCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:50:19.473165Z"},"content_sha256":"8087014b0a84201cebe5c377fdcab9a810ec06b3251c4537cb5b12856ccde538","schema_version":"1.0","event_id":"sha256:8087014b0a84201cebe5c377fdcab9a810ec06b3251c4537cb5b12856ccde538"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:TBICBQSV75HBHFRP3Z3J6J3JNP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The impact of additional scalar bosons at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alan S. Cornell, Biswarup Mukhopadhyaya, Bruce Mellado, Deepak Kar, Mukesh Kumar, Nabarun Chakrabarty, Robert Reed, Stefan von Buddenbrock, Tanumoy Mandal","submitted_at":"2016-03-03T18:15:58Z","abstract_excerpt":"In this study we consider an effective model by introducing two hypothetical real scalars, $H$ and $\\chi$ - a dark matter candidate, where the masses of these scalars are $2 m_h < m_H < 2 m_t$ and $m_\\chi \\approx m_h/2$ with $m_h$ and $m_t$ being the Standard Model Higgs boson and top quark masses respectively. A distortion in the transverse momentum distributions of $h$ in the intermediate region of the spectrum through the processes $p p \\to H \\to h\\chi\\chi$ could be observed in this model. An additional scalar, $S$, has been postulated to explain large $H \\to h\\chi\\chi$ branching ratios, as"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01208","kind":"arxiv","version":2},"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":"2026-05-18T00:47:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qjoLNf3J2OEnZk0jT9upKJdqGj0DWfUHtkRnoSTlu70/u5W1QtXj+ceVkKuZfM/Xshk0skkEJrcqB2GrMBieCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T06:50:19.473541Z"},"content_sha256":"0fcc11975ba93790034fe237ed2df30a907bb1f8de0b23c3befff96c9797763a","schema_version":"1.0","event_id":"sha256:0fcc11975ba93790034fe237ed2df30a907bb1f8de0b23c3befff96c9797763a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/bundle.json","state_url":"https://pith.science/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/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":"2026-05-28T06:50:19Z","links":{"resolver":"https://pith.science/pith/TBICBQSV75HBHFRP3Z3J6J3JNP","bundle":"https://pith.science/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/bundle.json","state":"https://pith.science/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TBICBQSV75HBHFRP3Z3J6J3JNP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:TBICBQSV75HBHFRP3Z3J6J3JNP","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":"5ea28fec8e5eb616e62a760a007b0737b431f07fcb7f2d8f440eed54e55424be","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-03T18:15:58Z","title_canon_sha256":"e0321b5ef5654be2954aca761a30ff4befbedb5d15f0a0b07040b977c0608e44"},"schema_version":"1.0","source":{"id":"1603.01208","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.01208","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"arxiv_version","alias_value":"1603.01208v2","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.01208","created_at":"2026-05-18T00:47:15Z"},{"alias_kind":"pith_short_12","alias_value":"TBICBQSV75HB","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_16","alias_value":"TBICBQSV75HBHFRP","created_at":"2026-05-18T12:30:44Z"},{"alias_kind":"pith_short_8","alias_value":"TBICBQSV","created_at":"2026-05-18T12:30:44Z"}],"graph_snapshots":[{"event_id":"sha256:0fcc11975ba93790034fe237ed2df30a907bb1f8de0b23c3befff96c9797763a","target":"graph","created_at":"2026-05-18T00:47:15Z","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 study we consider an effective model by introducing two hypothetical real scalars, $H$ and $\\chi$ - a dark matter candidate, where the masses of these scalars are $2 m_h < m_H < 2 m_t$ and $m_\\chi \\approx m_h/2$ with $m_h$ and $m_t$ being the Standard Model Higgs boson and top quark masses respectively. A distortion in the transverse momentum distributions of $h$ in the intermediate region of the spectrum through the processes $p p \\to H \\to h\\chi\\chi$ could be observed in this model. An additional scalar, $S$, has been postulated to explain large $H \\to h\\chi\\chi$ branching ratios, as","authors_text":"Alan S. Cornell, Biswarup Mukhopadhyaya, Bruce Mellado, Deepak Kar, Mukesh Kumar, Nabarun Chakrabarty, Robert Reed, Stefan von Buddenbrock, Tanumoy Mandal","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-03T18:15:58Z","title":"The impact of additional scalar bosons at the LHC"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.01208","kind":"arxiv","version":2},"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":"sha256:8087014b0a84201cebe5c377fdcab9a810ec06b3251c4537cb5b12856ccde538","target":"record","created_at":"2026-05-18T00:47:15Z","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":"5ea28fec8e5eb616e62a760a007b0737b431f07fcb7f2d8f440eed54e55424be","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-03-03T18:15:58Z","title_canon_sha256":"e0321b5ef5654be2954aca761a30ff4befbedb5d15f0a0b07040b977c0608e44"},"schema_version":"1.0","source":{"id":"1603.01208","kind":"arxiv","version":2}},"canonical_sha256":"985020c255ff4e13962fde769f27696bf8ff411cd9edf14f013aee55ef8b739d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"985020c255ff4e13962fde769f27696bf8ff411cd9edf14f013aee55ef8b739d","first_computed_at":"2026-05-18T00:47:15.347729Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:47:15.347729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Sz7NxZfRKRKQHjPE49LKn19PY63aCMvm+eefkaEgWZfvKdE4vf85UuwBtVChM+WSwDIqtHJAh54cBWWM1ahoBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:47:15.348437Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.01208","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8087014b0a84201cebe5c377fdcab9a810ec06b3251c4537cb5b12856ccde538","sha256:0fcc11975ba93790034fe237ed2df30a907bb1f8de0b23c3befff96c9797763a"],"state_sha256":"b281639a6d531fcf6870d373c5114b0203c4176127a86b9e88fe7f6721e0a7f8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FGM0ZDSdZbeORwKtdfuiSuJ1s1rMN4mo/dNNMeVpLFeVNq9XOr67qspwfGI92e+LYlFPBmk6eh8XuW1AW0f3Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T06:50:19.475655Z","bundle_sha256":"52f42d413b74b976c9c6dea53fed1b1f1e474a73c0a4353645850031421d4a8c"}}