{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:SNNDVXWR76S4V2LFLHAUKMZ4EC","short_pith_number":"pith:SNNDVXWR","schema_version":"1.0","canonical_sha256":"935a3aded1ffa5cae96559c145333c2083747a7721b2ccd6527b1b4066ba3c4f","source":{"kind":"arxiv","id":"1510.08959","version":1},"attestation_state":"computed","paper":{"title":"Polarization of the top quark as a probe of its chromomagnetic and chromoelectric couplings in single-top production at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anthony W. Thomas, Pankaj Sharma, Saurabh D. Rindani","submitted_at":"2015-10-30T03:13:34Z","abstract_excerpt":"We study the sensitivity of the Large Hadron Collider (LHC) to top quark chromomagnetic (CMDM) and chromoelectric (CEDM) dipole moments and $Wtb$ effective couplings in single-top production in association with a $W^-$ boson, followed by semileptonic decay of the top. We calculate the top polarization and the effects of these anomalous couplings on it at two centre-of-mass (cm) energies, 8 TeV and 14 TeV. As a measure of top polarization, we look at decay-lepton angular distributions in the laboratory frame, without requiring reconstruction of the rest frame of the top, and study the effect of"},"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":"1510.08959","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-10-30T03:13:34Z","cross_cats_sorted":[],"title_canon_sha256":"81b4cde88278b42ccb92bc71ed3277ffbbe37137d97f4ab98fa2f3128796191d","abstract_canon_sha256":"b82de3ee8f88299d24b028e0ba75b1d678a7f947073bedac7539555a96f2adc4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:24.016179Z","signature_b64":"xtmh2AhU26wO6lF2rE+4j2gnEJNL5WqH4IIt60msxn2S0VcW9Lp/75eIYy9+I9KmcGr1jet5I+Z15PSOLqbzAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"935a3aded1ffa5cae96559c145333c2083747a7721b2ccd6527b1b4066ba3c4f","last_reissued_at":"2026-05-18T01:28:24.015588Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:24.015588Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Polarization of the top quark as a probe of its chromomagnetic and chromoelectric couplings in single-top production at the Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anthony W. Thomas, Pankaj Sharma, Saurabh D. Rindani","submitted_at":"2015-10-30T03:13:34Z","abstract_excerpt":"We study the sensitivity of the Large Hadron Collider (LHC) to top quark chromomagnetic (CMDM) and chromoelectric (CEDM) dipole moments and $Wtb$ effective couplings in single-top production in association with a $W^-$ boson, followed by semileptonic decay of the top. We calculate the top polarization and the effects of these anomalous couplings on it at two centre-of-mass (cm) energies, 8 TeV and 14 TeV. As a measure of top polarization, we look at decay-lepton angular distributions in the laboratory frame, without requiring reconstruction of the rest frame of the top, and study the effect of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.08959","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":"1510.08959","created_at":"2026-05-18T01:28:24.015672+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.08959v1","created_at":"2026-05-18T01:28:24.015672+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.08959","created_at":"2026-05-18T01:28:24.015672+00:00"},{"alias_kind":"pith_short_12","alias_value":"SNNDVXWR76S4","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_16","alias_value":"SNNDVXWR76S4V2LF","created_at":"2026-05-18T12:29:42.218222+00:00"},{"alias_kind":"pith_short_8","alias_value":"SNNDVXWR","created_at":"2026-05-18T12:29:42.218222+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC","json":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC.json","graph_json":"https://pith.science/api/pith-number/SNNDVXWR76S4V2LFLHAUKMZ4EC/graph.json","events_json":"https://pith.science/api/pith-number/SNNDVXWR76S4V2LFLHAUKMZ4EC/events.json","paper":"https://pith.science/paper/SNNDVXWR"},"agent_actions":{"view_html":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC","download_json":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC.json","view_paper":"https://pith.science/paper/SNNDVXWR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.08959&json=true","fetch_graph":"https://pith.science/api/pith-number/SNNDVXWR76S4V2LFLHAUKMZ4EC/graph.json","fetch_events":"https://pith.science/api/pith-number/SNNDVXWR76S4V2LFLHAUKMZ4EC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC/action/storage_attestation","attest_author":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC/action/author_attestation","sign_citation":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC/action/citation_signature","submit_replication":"https://pith.science/pith/SNNDVXWR76S4V2LFLHAUKMZ4EC/action/replication_record"}},"created_at":"2026-05-18T01:28:24.015672+00:00","updated_at":"2026-05-18T01:28:24.015672+00:00"}