{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:OL7YC3ZS27CTOGNCBK3H5Q5RPK","short_pith_number":"pith:OL7YC3ZS","schema_version":"1.0","canonical_sha256":"72ff816f32d7c53719a20ab67ec3b17a81e24e0a5af52c0a96b671e932bf0ffb","source":{"kind":"arxiv","id":"2502.01775","version":2},"attestation_state":"computed","paper":{"title":"Zero Modes on the Light Front","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"J.R. Hiller, S.S. Chabysheva","submitted_at":"2025-02-03T19:28:46Z","abstract_excerpt":"Modes with zero longitudinal light-front momentum (zero modes) do have roles to play in the analysis of light-front field theories. These range from improvements in convergence for numerical calculations to implications for the light-front vacuum and beyond to fundamental issues in the connection with equal-time quantization. In particular, the discrepancy in values of the critical coupling for $\\phi^4_{1+1}$ theory, between equal-time and light-front quantizations, would appear to be resolvable with the proper treatment of zero modes and near-zero modes. We provide a survey of these issues an"},"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":"2502.01775","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-02-03T19:28:46Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"4880ce965027d3f6554e525dc30d4cdce9a6494897bdcb2b69fdd4aa842ae4e0","abstract_canon_sha256":"6cbda5642e68b6cfbbe0c0c23c357e5868a6b84537bc29cfd8d84a8628daac14"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:22:36.260012Z","signature_b64":"NPpkctlN8JVUD0M2bkpF5UllnYEfDi4T7iQ2oAcZjzjBtBU5DyHLIAcAb6K2Q6VmpKxGX2Nm/4cdN1Ju8FFyBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72ff816f32d7c53719a20ab67ec3b17a81e24e0a5af52c0a96b671e932bf0ffb","last_reissued_at":"2026-07-05T11:22:36.258267Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:22:36.258267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Zero Modes on the Light Front","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"J.R. Hiller, S.S. Chabysheva","submitted_at":"2025-02-03T19:28:46Z","abstract_excerpt":"Modes with zero longitudinal light-front momentum (zero modes) do have roles to play in the analysis of light-front field theories. These range from improvements in convergence for numerical calculations to implications for the light-front vacuum and beyond to fundamental issues in the connection with equal-time quantization. In particular, the discrepancy in values of the critical coupling for $\\phi^4_{1+1}$ theory, between equal-time and light-front quantizations, would appear to be resolvable with the proper treatment of zero modes and near-zero modes. We provide a survey of these issues an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.01775","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/2502.01775/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":"2502.01775","created_at":"2026-07-05T11:22:36.259417+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.01775v2","created_at":"2026-07-05T11:22:36.259417+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.01775","created_at":"2026-07-05T11:22:36.259417+00:00"},{"alias_kind":"pith_short_12","alias_value":"OL7YC3ZS27CT","created_at":"2026-07-05T11:22:36.259417+00:00"},{"alias_kind":"pith_short_16","alias_value":"OL7YC3ZS27CTOGNC","created_at":"2026-07-05T11:22:36.259417+00:00"},{"alias_kind":"pith_short_8","alias_value":"OL7YC3ZS","created_at":"2026-07-05T11:22:36.259417+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.24699","citing_title":"Second-order effective renormalized Hamiltonian of Quantum Chromodynamics","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK","json":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK.json","graph_json":"https://pith.science/api/pith-number/OL7YC3ZS27CTOGNCBK3H5Q5RPK/graph.json","events_json":"https://pith.science/api/pith-number/OL7YC3ZS27CTOGNCBK3H5Q5RPK/events.json","paper":"https://pith.science/paper/OL7YC3ZS"},"agent_actions":{"view_html":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK","download_json":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK.json","view_paper":"https://pith.science/paper/OL7YC3ZS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.01775&json=true","fetch_graph":"https://pith.science/api/pith-number/OL7YC3ZS27CTOGNCBK3H5Q5RPK/graph.json","fetch_events":"https://pith.science/api/pith-number/OL7YC3ZS27CTOGNCBK3H5Q5RPK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK/action/storage_attestation","attest_author":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK/action/author_attestation","sign_citation":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK/action/citation_signature","submit_replication":"https://pith.science/pith/OL7YC3ZS27CTOGNCBK3H5Q5RPK/action/replication_record"}},"created_at":"2026-07-05T11:22:36.259417+00:00","updated_at":"2026-07-05T11:22:36.259417+00:00"}