{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:ZACSYNMMUP5NP3LF5IG4BVAJ43","short_pith_number":"pith:ZACSYNMM","schema_version":"1.0","canonical_sha256":"c8052c358ca3fad7ed65ea0dc0d409e6f3de6563348bbe33ee66809cf1a42236","source":{"kind":"arxiv","id":"2302.12005","version":2},"attestation_state":"computed","paper":{"title":"Constraining Lorentz Invariance Violation with Next-Generation Long-Baseline Experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","physics.ins-det"],"primary_cat":"hep-ph","authors_text":"Pragyanprasu Swain, Sadashiv Sahoo, Sanjib Kumar Agarwalla, Sudipta Das","submitted_at":"2023-02-23T13:24:32Z","abstract_excerpt":"Unified theories such as string theory and loop quantum gravity allow the Lorentz Invariance Violation (LIV) at the Planck Scale ($M_P \\sim 10^{19}$ GeV). Using an effective field theory, this effect can be observed at low energies in terms of new interactions with a strength of $\\sim 1/M_P$. These new interactions contain operators with LIV coefficients which can be CPT-violating or CPT-conserving. In this work, we study in detail how these LIV parameters modify the transition probabilities in the next-generation long-baseline experiments, DUNE and T2HK. We evaluate the sensitivities of these"},"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":"2302.12005","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-02-23T13:24:32Z","cross_cats_sorted":["hep-ex","physics.ins-det"],"title_canon_sha256":"28ae5bf11bd545a3e29f0e524e67ce3b4efed38d1f023b92fd89535d12d93391","abstract_canon_sha256":"5d5cf75f7c277da26225e6a65d2a98bc9c0935530396779965e89174ea59cfab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:40:51.313274Z","signature_b64":"vkxeuZMbz4+0DVSVVDyL3y7ONwSBJPDeBFMURdXWPdNtrAF4IJ2eZIJADIoyrSMI4xFKp5wE7oBFR7zNJ6K2CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c8052c358ca3fad7ed65ea0dc0d409e6f3de6563348bbe33ee66809cf1a42236","last_reissued_at":"2026-07-05T06:40:51.312713Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:40:51.312713Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraining Lorentz Invariance Violation with Next-Generation Long-Baseline Experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","physics.ins-det"],"primary_cat":"hep-ph","authors_text":"Pragyanprasu Swain, Sadashiv Sahoo, Sanjib Kumar Agarwalla, Sudipta Das","submitted_at":"2023-02-23T13:24:32Z","abstract_excerpt":"Unified theories such as string theory and loop quantum gravity allow the Lorentz Invariance Violation (LIV) at the Planck Scale ($M_P \\sim 10^{19}$ GeV). Using an effective field theory, this effect can be observed at low energies in terms of new interactions with a strength of $\\sim 1/M_P$. These new interactions contain operators with LIV coefficients which can be CPT-violating or CPT-conserving. In this work, we study in detail how these LIV parameters modify the transition probabilities in the next-generation long-baseline experiments, DUNE and T2HK. We evaluate the sensitivities of these"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.12005","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/2302.12005/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":"2302.12005","created_at":"2026-07-05T06:40:51.312790+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.12005v2","created_at":"2026-07-05T06:40:51.312790+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.12005","created_at":"2026-07-05T06:40:51.312790+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZACSYNMMUP5N","created_at":"2026-07-05T06:40:51.312790+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZACSYNMMUP5NP3LF","created_at":"2026-07-05T06:40:51.312790+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZACSYNMM","created_at":"2026-07-05T06:40:51.312790+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06513","citing_title":"Interplay of CPT-Violating and CPT-Conserving Lorentz Invariance Violation at DUNE","ref_index":11,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43","json":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43.json","graph_json":"https://pith.science/api/pith-number/ZACSYNMMUP5NP3LF5IG4BVAJ43/graph.json","events_json":"https://pith.science/api/pith-number/ZACSYNMMUP5NP3LF5IG4BVAJ43/events.json","paper":"https://pith.science/paper/ZACSYNMM"},"agent_actions":{"view_html":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43","download_json":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43.json","view_paper":"https://pith.science/paper/ZACSYNMM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.12005&json=true","fetch_graph":"https://pith.science/api/pith-number/ZACSYNMMUP5NP3LF5IG4BVAJ43/graph.json","fetch_events":"https://pith.science/api/pith-number/ZACSYNMMUP5NP3LF5IG4BVAJ43/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43/action/storage_attestation","attest_author":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43/action/author_attestation","sign_citation":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43/action/citation_signature","submit_replication":"https://pith.science/pith/ZACSYNMMUP5NP3LF5IG4BVAJ43/action/replication_record"}},"created_at":"2026-07-05T06:40:51.312790+00:00","updated_at":"2026-07-05T06:40:51.312790+00:00"}