{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:6N7XUEFJFLHJJ53JC36MZXW6OQ","short_pith_number":"pith:6N7XUEFJ","schema_version":"1.0","canonical_sha256":"f37f7a10a92ace94f76916fcccdede7429e8bcf3c9e9f0d768574de952e38f2f","source":{"kind":"arxiv","id":"1211.3057","version":3},"attestation_state":"computed","paper":{"title":"Lattice evidence for the family of decoupling solutions of Landau gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andre Sternbeck, Michael M\\\"uller-Preussker","submitted_at":"2012-11-13T17:28:46Z","abstract_excerpt":"We show that the low-momentum behavior of the lattice Landau-gauge gluon and ghost propagators is sensitive to the lowest non-trivial eigenvalue (\\lambda_1) of the Faddeev-Popov operator. If the gauge fixing favors Gribov copies with small \\lambda_1 the ghost dressing function rises more rapidly towards zero momentum than on copies with large \\lambda_1. This effect is seen for momenta below 1 GeV, and interestingly also for the gluon propagator at momenta below 0.2 GeV: For large \\lambda_1 the gluon propagator levels out to a lower value at zero momentum than for small \\lambda_1. For momenta a"},"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":"1211.3057","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-11-13T17:28:46Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"cccc1bf16eb68c4842a3769e9e347e3abbefe5d29877f0f505fea1b54b8d1fa8","abstract_canon_sha256":"c805ac0933df2ebca26ac38ce652350f0d667c987b5a0de4107217304046956c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:12:09.036451Z","signature_b64":"RIF7TCw8cgwUcOD2k+F0FhmJUkUXCdcIIETXdUQaKgx4GBbmWTu1acveTUEuuCmN1vfR4Q7FnSdOKu1EKUc2DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f37f7a10a92ace94f76916fcccdede7429e8bcf3c9e9f0d768574de952e38f2f","last_reissued_at":"2026-05-18T03:12:09.035590Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:12:09.035590Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lattice evidence for the family of decoupling solutions of Landau gauge Yang-Mills theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andre Sternbeck, Michael M\\\"uller-Preussker","submitted_at":"2012-11-13T17:28:46Z","abstract_excerpt":"We show that the low-momentum behavior of the lattice Landau-gauge gluon and ghost propagators is sensitive to the lowest non-trivial eigenvalue (\\lambda_1) of the Faddeev-Popov operator. If the gauge fixing favors Gribov copies with small \\lambda_1 the ghost dressing function rises more rapidly towards zero momentum than on copies with large \\lambda_1. This effect is seen for momenta below 1 GeV, and interestingly also for the gluon propagator at momenta below 0.2 GeV: For large \\lambda_1 the gluon propagator levels out to a lower value at zero momentum than for small \\lambda_1. For momenta a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.3057","kind":"arxiv","version":3},"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":"1211.3057","created_at":"2026-05-18T03:12:09.035704+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.3057v3","created_at":"2026-05-18T03:12:09.035704+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.3057","created_at":"2026-05-18T03:12:09.035704+00:00"},{"alias_kind":"pith_short_12","alias_value":"6N7XUEFJFLHJ","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"6N7XUEFJFLHJJ53J","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"6N7XUEFJ","created_at":"2026-05-18T12:26:56.085431+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/6N7XUEFJFLHJJ53JC36MZXW6OQ","json":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ.json","graph_json":"https://pith.science/api/pith-number/6N7XUEFJFLHJJ53JC36MZXW6OQ/graph.json","events_json":"https://pith.science/api/pith-number/6N7XUEFJFLHJJ53JC36MZXW6OQ/events.json","paper":"https://pith.science/paper/6N7XUEFJ"},"agent_actions":{"view_html":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ","download_json":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ.json","view_paper":"https://pith.science/paper/6N7XUEFJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.3057&json=true","fetch_graph":"https://pith.science/api/pith-number/6N7XUEFJFLHJJ53JC36MZXW6OQ/graph.json","fetch_events":"https://pith.science/api/pith-number/6N7XUEFJFLHJJ53JC36MZXW6OQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ/action/storage_attestation","attest_author":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ/action/author_attestation","sign_citation":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ/action/citation_signature","submit_replication":"https://pith.science/pith/6N7XUEFJFLHJJ53JC36MZXW6OQ/action/replication_record"}},"created_at":"2026-05-18T03:12:09.035704+00:00","updated_at":"2026-05-18T03:12:09.035704+00:00"}