{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:6HIKEUH7YZ5XURVRHALIZN2MMN","short_pith_number":"pith:6HIKEUH7","schema_version":"1.0","canonical_sha256":"f1d0a250ffc67b7a46b138168cb74c635b75911a770560f76fcce972fe8eb7d1","source":{"kind":"arxiv","id":"2006.16363","version":2},"attestation_state":"computed","paper":{"title":"Feasibility studies for the measurement of time-like proton electromagnetic form factors from $\\bar{p}p \\rightarrow \\mu^+\\mu^-$ at $\\overline{\\textrm{P}}\\textrm{ANDA}$ at FAIR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The PANDA Collaboration","submitted_at":"2020-06-29T20:29:47Z","abstract_excerpt":"This paper reports on Monte Carlo simulation results for future measurements of time-like proton electromagnetic form factors, $|G_{E}|$ and $|G_{M}|$, using the $\\bar{p} p \\rightarrow \\mu^{+} \\mu^{-}$ reaction at $\\overline{\\textrm{P}}\\textrm{ANDA}$ (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at $\\overline{\\textrm{P}}\\textrm{ANDA}$, using an analysis of simulated data within the PandaRoot software framework. T"},"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":"2006.16363","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2020-06-29T20:29:47Z","cross_cats_sorted":[],"title_canon_sha256":"ac8f270b7f85a7667661e5a21fce15e5c6e2e737a5d648566404d5532870e882","abstract_canon_sha256":"1eee6f053bce32a150713e72f68412e2ce5e0dd51832cf668486dbd837520423"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:15:26.983957Z","signature_b64":"qJm290vFRCJv3+Pso7dnO3fzCpNo9j05Rcc8pe/WJIge66oTq5kKyM3/K8zp9ozwddRc5QgKZEQp9aoXDQYdAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f1d0a250ffc67b7a46b138168cb74c635b75911a770560f76fcce972fe8eb7d1","last_reissued_at":"2026-07-05T01:15:26.983528Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:15:26.983528Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Feasibility studies for the measurement of time-like proton electromagnetic form factors from $\\bar{p}p \\rightarrow \\mu^+\\mu^-$ at $\\overline{\\textrm{P}}\\textrm{ANDA}$ at FAIR","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The PANDA Collaboration","submitted_at":"2020-06-29T20:29:47Z","abstract_excerpt":"This paper reports on Monte Carlo simulation results for future measurements of time-like proton electromagnetic form factors, $|G_{E}|$ and $|G_{M}|$, using the $\\bar{p} p \\rightarrow \\mu^{+} \\mu^{-}$ reaction at $\\overline{\\textrm{P}}\\textrm{ANDA}$ (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at $\\overline{\\textrm{P}}\\textrm{ANDA}$, using an analysis of simulated data within the PandaRoot software framework. T"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2006.16363","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2006.16363/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2006.16363","created_at":"2026-07-05T01:15:26.983595+00:00"},{"alias_kind":"arxiv_version","alias_value":"2006.16363v2","created_at":"2026-07-05T01:15:26.983595+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2006.16363","created_at":"2026-07-05T01:15:26.983595+00:00"},{"alias_kind":"pith_short_12","alias_value":"6HIKEUH7YZ5X","created_at":"2026-07-05T01:15:26.983595+00:00"},{"alias_kind":"pith_short_16","alias_value":"6HIKEUH7YZ5XURVR","created_at":"2026-07-05T01:15:26.983595+00:00"},{"alias_kind":"pith_short_8","alias_value":"6HIKEUH7","created_at":"2026-07-05T01:15:26.983595+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06459","citing_title":"Input-to-State Stability Certification via Projection Residuals for Koopman Learning Control of Nonlinear Repetitive Systems","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN","json":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN.json","graph_json":"https://pith.science/api/pith-number/6HIKEUH7YZ5XURVRHALIZN2MMN/graph.json","events_json":"https://pith.science/api/pith-number/6HIKEUH7YZ5XURVRHALIZN2MMN/events.json","paper":"https://pith.science/paper/6HIKEUH7"},"agent_actions":{"view_html":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN","download_json":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN.json","view_paper":"https://pith.science/paper/6HIKEUH7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2006.16363&json=true","fetch_graph":"https://pith.science/api/pith-number/6HIKEUH7YZ5XURVRHALIZN2MMN/graph.json","fetch_events":"https://pith.science/api/pith-number/6HIKEUH7YZ5XURVRHALIZN2MMN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN/action/storage_attestation","attest_author":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN/action/author_attestation","sign_citation":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN/action/citation_signature","submit_replication":"https://pith.science/pith/6HIKEUH7YZ5XURVRHALIZN2MMN/action/replication_record"}},"created_at":"2026-07-05T01:15:26.983595+00:00","updated_at":"2026-07-05T01:15:26.983595+00:00"}