{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:AU32JZFDQCT7LDKSCJXHTFPLTL","short_pith_number":"pith:AU32JZFD","schema_version":"1.0","canonical_sha256":"0537a4e4a380a7f58d52126e7995eb9afe11096eb25cc4042a1f00877fcaa4aa","source":{"kind":"arxiv","id":"1410.6970","version":2},"attestation_state":"computed","paper":{"title":"New Physics Search with Precision Experiments: Theory Input","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A. Aleksejevs, S. Barkanova, S. Wu, V. Zykunov","submitted_at":"2014-10-25T22:48:50Z","abstract_excerpt":"The best way to search for new physics is by using a diverse set of probes - not just experiments at the energy and the cosmic frontiers, but also the low-energy measurements relying on high precision and high luminosity. One example of such ultra-precision experiments is the MOLLER experiment planned at JLab, which will measure the parity-violating electron-electron scattering asymmetry and allow a determination of the weak mixing angle with a factor of five improvement in precision over its predecessor, E-158. At this precision, any inconsistency with the Standard Model should signal new phy"},"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":"1410.6970","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-10-25T22:48:50Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"dea42a65cba3bf08259824a17e4d72982a5b07eeffc569f6e19202e1293c480e","abstract_canon_sha256":"d88757e9d165360e10aeb11f737f1151653679c503697184b88edfd98518f7eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:15:44.598481Z","signature_b64":"bBN1wXY2TGDBjx4XNadHzp9G4bZmqWKX1dchyqq8Jzv3aVERgHUAT4a9OyHpt+46GFPbUMUIAw24Vj7FkoquAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0537a4e4a380a7f58d52126e7995eb9afe11096eb25cc4042a1f00877fcaa4aa","last_reissued_at":"2026-07-05T00:15:44.598061Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:15:44.598061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New Physics Search with Precision Experiments: Theory Input","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A. Aleksejevs, S. Barkanova, S. Wu, V. Zykunov","submitted_at":"2014-10-25T22:48:50Z","abstract_excerpt":"The best way to search for new physics is by using a diverse set of probes - not just experiments at the energy and the cosmic frontiers, but also the low-energy measurements relying on high precision and high luminosity. One example of such ultra-precision experiments is the MOLLER experiment planned at JLab, which will measure the parity-violating electron-electron scattering asymmetry and allow a determination of the weak mixing angle with a factor of five improvement in precision over its predecessor, E-158. At this precision, any inconsistency with the Standard Model should signal new phy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.6970","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/1410.6970/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":"1410.6970","created_at":"2026-07-05T00:15:44.598115+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.6970v2","created_at":"2026-07-05T00:15:44.598115+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.6970","created_at":"2026-07-05T00:15:44.598115+00:00"},{"alias_kind":"pith_short_12","alias_value":"AU32JZFDQCT7","created_at":"2026-07-05T00:15:44.598115+00:00"},{"alias_kind":"pith_short_16","alias_value":"AU32JZFDQCT7LDKS","created_at":"2026-07-05T00:15:44.598115+00:00"},{"alias_kind":"pith_short_8","alias_value":"AU32JZFD","created_at":"2026-07-05T00:15:44.598115+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/AU32JZFDQCT7LDKSCJXHTFPLTL","json":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL.json","graph_json":"https://pith.science/api/pith-number/AU32JZFDQCT7LDKSCJXHTFPLTL/graph.json","events_json":"https://pith.science/api/pith-number/AU32JZFDQCT7LDKSCJXHTFPLTL/events.json","paper":"https://pith.science/paper/AU32JZFD"},"agent_actions":{"view_html":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL","download_json":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL.json","view_paper":"https://pith.science/paper/AU32JZFD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.6970&json=true","fetch_graph":"https://pith.science/api/pith-number/AU32JZFDQCT7LDKSCJXHTFPLTL/graph.json","fetch_events":"https://pith.science/api/pith-number/AU32JZFDQCT7LDKSCJXHTFPLTL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL/action/storage_attestation","attest_author":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL/action/author_attestation","sign_citation":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL/action/citation_signature","submit_replication":"https://pith.science/pith/AU32JZFDQCT7LDKSCJXHTFPLTL/action/replication_record"}},"created_at":"2026-07-05T00:15:44.598115+00:00","updated_at":"2026-07-05T00:15:44.598115+00:00"}