{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:M7WDGEXOPHQD75M7MCKHXSMMMO","short_pith_number":"pith:M7WDGEXO","schema_version":"1.0","canonical_sha256":"67ec3312ee79e03ff59f60947bc98c63ade83c029931a443f847b80a52acec23","source":{"kind":"arxiv","id":"1608.07500","version":1},"attestation_state":"computed","paper":{"title":"Search for Mono-Higgs Signals at the LHC in the B-L Supersymmetric Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Hammad, S. Khalil, S. Moretti, W. Abdallah","submitted_at":"2016-08-26T16:03:49Z","abstract_excerpt":"We study mono-Higgs signatures emerging in the $B-L$ supersymmetric standard model induced by new channels not present in the minimal supersymmetric standard model, i.e., via topologies in which the mediator is either a heavy $Z'$, with mass of ${\\cal O}(2~{\\rm TeV})$, or an intermediate $h'$ (the lightest CP-even Higgs state of $B-L$ origin), with mass of ${\\cal O}(0.2~{\\rm TeV})$. The mono-Higgs probe considered is the SM-like Higgs state recently discovered at the large hadron collider, so as to enforce its mass reconstruction for background reduction purposes. With this in mind, its two cl"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1608.07500","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-26T16:03:49Z","cross_cats_sorted":[],"title_canon_sha256":"3a50d261e9a29edcbc993af698c4317b54dfa8411a8550da7a2adf59e6f7ab92","abstract_canon_sha256":"46cfa20a7962687b88c21c1aff24ddc53706223672a0e3e3da60f94508a7709c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:50.138962Z","signature_b64":"A2KzVgrR0ODpVOQCQrL9MgaWNabIUkF7bsHWUt7Yomrkmb9LWIHqACd9nyNqQyuoRPMQYXdaRTqkxaIfQTmOBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67ec3312ee79e03ff59f60947bc98c63ade83c029931a443f847b80a52acec23","last_reissued_at":"2026-05-18T00:47:50.138235Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:50.138235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for Mono-Higgs Signals at the LHC in the B-L Supersymmetric Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Hammad, S. Khalil, S. Moretti, W. Abdallah","submitted_at":"2016-08-26T16:03:49Z","abstract_excerpt":"We study mono-Higgs signatures emerging in the $B-L$ supersymmetric standard model induced by new channels not present in the minimal supersymmetric standard model, i.e., via topologies in which the mediator is either a heavy $Z'$, with mass of ${\\cal O}(2~{\\rm TeV})$, or an intermediate $h'$ (the lightest CP-even Higgs state of $B-L$ origin), with mass of ${\\cal O}(0.2~{\\rm TeV})$. The mono-Higgs probe considered is the SM-like Higgs state recently discovered at the large hadron collider, so as to enforce its mass reconstruction for background reduction purposes. With this in mind, its two cl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.07500","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1608.07500","created_at":"2026-05-18T00:47:50.138357+00:00"},{"alias_kind":"arxiv_version","alias_value":"1608.07500v1","created_at":"2026-05-18T00:47:50.138357+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.07500","created_at":"2026-05-18T00:47:50.138357+00:00"},{"alias_kind":"pith_short_12","alias_value":"M7WDGEXOPHQD","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"M7WDGEXOPHQD75M7","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"M7WDGEXO","created_at":"2026-05-18T12:30:29.479603+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.01060","citing_title":"$S, T, U$ Parameters in The B-LSSM","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2604.23038","citing_title":"Mono-Z' Signatures in the B-L Supersymmetric Standard Model at the LHC","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO","json":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO.json","graph_json":"https://pith.science/api/pith-number/M7WDGEXOPHQD75M7MCKHXSMMMO/graph.json","events_json":"https://pith.science/api/pith-number/M7WDGEXOPHQD75M7MCKHXSMMMO/events.json","paper":"https://pith.science/paper/M7WDGEXO"},"agent_actions":{"view_html":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO","download_json":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO.json","view_paper":"https://pith.science/paper/M7WDGEXO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1608.07500&json=true","fetch_graph":"https://pith.science/api/pith-number/M7WDGEXOPHQD75M7MCKHXSMMMO/graph.json","fetch_events":"https://pith.science/api/pith-number/M7WDGEXOPHQD75M7MCKHXSMMMO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO/action/storage_attestation","attest_author":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO/action/author_attestation","sign_citation":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO/action/citation_signature","submit_replication":"https://pith.science/pith/M7WDGEXOPHQD75M7MCKHXSMMMO/action/replication_record"}},"created_at":"2026-05-18T00:47:50.138357+00:00","updated_at":"2026-05-18T00:47:50.138357+00:00"}