{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:VA2JVISBVGVELMP36CVHFFFMQ5","short_pith_number":"pith:VA2JVISB","canonical_record":{"source":{"id":"1302.5943","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-24T19:26:58Z","cross_cats_sorted":[],"title_canon_sha256":"79a144a2a491a15dda8c4c8b63794bff3520b51c0a92ccbbdf674e8a6ccc19e8","abstract_canon_sha256":"23ca5b10565ba50d6fe109dd912ad9479136e4e289c63fd1119629a2eb221541"},"schema_version":"1.0"},"canonical_sha256":"a8349aa241a9aa45b1fbf0aa7294ac8768cc30926cc9f2e7e4eca3007eb2dfe0","source":{"kind":"arxiv","id":"1302.5943","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.5943","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"arxiv_version","alias_value":"1302.5943v2","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.5943","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"pith_short_12","alias_value":"VA2JVISBVGVE","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VA2JVISBVGVELMP3","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VA2JVISB","created_at":"2026-05-18T12:28:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:VA2JVISBVGVELMP36CVHFFFMQ5","target":"record","payload":{"canonical_record":{"source":{"id":"1302.5943","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-24T19:26:58Z","cross_cats_sorted":[],"title_canon_sha256":"79a144a2a491a15dda8c4c8b63794bff3520b51c0a92ccbbdf674e8a6ccc19e8","abstract_canon_sha256":"23ca5b10565ba50d6fe109dd912ad9479136e4e289c63fd1119629a2eb221541"},"schema_version":"1.0"},"canonical_sha256":"a8349aa241a9aa45b1fbf0aa7294ac8768cc30926cc9f2e7e4eca3007eb2dfe0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:30:49.539534Z","signature_b64":"XgTd8osAsUQfjfEqjb0IWX4WxoibtJz7EBPAO/nf01ZMcCaDkRDHAPlEzRXhpEJB7tEziNpj0dlcJxHFXlFuCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a8349aa241a9aa45b1fbf0aa7294ac8768cc30926cc9f2e7e4eca3007eb2dfe0","last_reissued_at":"2026-05-18T01:30:49.539007Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:30:49.539007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1302.5943","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:30:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rkYzoSse5ClmsLUP00fM+jfBnzgAeSVNOJzkf/5plBZM3GJuFW8N7/vbTFP/K7pPfov7wAtJDuDCq/3Utr2sDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T10:51:31.377515Z"},"content_sha256":"bedd1ffac2c6337cd4a1c8e5098bde93ba4c9c32da98a1b93192c802a3248ac9","schema_version":"1.0","event_id":"sha256:bedd1ffac2c6337cd4a1c8e5098bde93ba4c9c32da98a1b93192c802a3248ac9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:VA2JVISBVGVELMP36CVHFFFMQ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Landau gauge ghost propagator and running coupling in SU(2) lattice gauge theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"C. Litwinski, E.-M. Ilgenfritz, M. Muller-Preussker, V. G. Bornyakov, V. K. Mitrjushkin","submitted_at":"2013-02-24T19:26:58Z","abstract_excerpt":"We study finite (physical) volume and scaling violation effects of the Landau gauge ghost propagator as well as of the running coupling $\\alpha_s(p)$ in the $SU(2)$ lattice gauge theory. We consider lattices with physical linear sizes between $aL \\simeq 3$ fm and $7$ fm and values of lattice spacing between $a=0.2$ fm and $0.07$ fm. To fix the gauge we apply an efficient gauge fixing method aimed at finding extrema as close as possible to the global maximum of the gauge functional. We find finite volume effects to be small for the lattice size $aL \\simeq 3$ fm at momenta $|p|\\, \\ge \\, 0.6$ GeV"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.5943","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:30:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w1y8Mgq31RtFgaLXjSQo/cCKrc2J8ItgdypXz9hvaTp808YsEEr09/9R4u/PIPrnV2f1igTVRmP5Y7aUXj3eCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T10:51:31.378196Z"},"content_sha256":"b2153f44b2e3013ff4ff1b2d8f52480fa40ab4ccd8228cc3c726c9092a7c3180","schema_version":"1.0","event_id":"sha256:b2153f44b2e3013ff4ff1b2d8f52480fa40ab4ccd8228cc3c726c9092a7c3180"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VA2JVISBVGVELMP36CVHFFFMQ5/bundle.json","state_url":"https://pith.science/pith/VA2JVISBVGVELMP36CVHFFFMQ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VA2JVISBVGVELMP36CVHFFFMQ5/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-27T10:51:31Z","links":{"resolver":"https://pith.science/pith/VA2JVISBVGVELMP36CVHFFFMQ5","bundle":"https://pith.science/pith/VA2JVISBVGVELMP36CVHFFFMQ5/bundle.json","state":"https://pith.science/pith/VA2JVISBVGVELMP36CVHFFFMQ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VA2JVISBVGVELMP36CVHFFFMQ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:VA2JVISBVGVELMP36CVHFFFMQ5","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"23ca5b10565ba50d6fe109dd912ad9479136e4e289c63fd1119629a2eb221541","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-24T19:26:58Z","title_canon_sha256":"79a144a2a491a15dda8c4c8b63794bff3520b51c0a92ccbbdf674e8a6ccc19e8"},"schema_version":"1.0","source":{"id":"1302.5943","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.5943","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"arxiv_version","alias_value":"1302.5943v2","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.5943","created_at":"2026-05-18T01:30:49Z"},{"alias_kind":"pith_short_12","alias_value":"VA2JVISBVGVE","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_16","alias_value":"VA2JVISBVGVELMP3","created_at":"2026-05-18T12:28:04Z"},{"alias_kind":"pith_short_8","alias_value":"VA2JVISB","created_at":"2026-05-18T12:28:04Z"}],"graph_snapshots":[{"event_id":"sha256:b2153f44b2e3013ff4ff1b2d8f52480fa40ab4ccd8228cc3c726c9092a7c3180","target":"graph","created_at":"2026-05-18T01:30:49Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study finite (physical) volume and scaling violation effects of the Landau gauge ghost propagator as well as of the running coupling $\\alpha_s(p)$ in the $SU(2)$ lattice gauge theory. We consider lattices with physical linear sizes between $aL \\simeq 3$ fm and $7$ fm and values of lattice spacing between $a=0.2$ fm and $0.07$ fm. To fix the gauge we apply an efficient gauge fixing method aimed at finding extrema as close as possible to the global maximum of the gauge functional. We find finite volume effects to be small for the lattice size $aL \\simeq 3$ fm at momenta $|p|\\, \\ge \\, 0.6$ GeV","authors_text":"C. Litwinski, E.-M. Ilgenfritz, M. Muller-Preussker, V. G. Bornyakov, V. K. Mitrjushkin","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-24T19:26:58Z","title":"Landau gauge ghost propagator and running coupling in SU(2) lattice gauge theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.5943","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:bedd1ffac2c6337cd4a1c8e5098bde93ba4c9c32da98a1b93192c802a3248ac9","target":"record","created_at":"2026-05-18T01:30:49Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"23ca5b10565ba50d6fe109dd912ad9479136e4e289c63fd1119629a2eb221541","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-02-24T19:26:58Z","title_canon_sha256":"79a144a2a491a15dda8c4c8b63794bff3520b51c0a92ccbbdf674e8a6ccc19e8"},"schema_version":"1.0","source":{"id":"1302.5943","kind":"arxiv","version":2}},"canonical_sha256":"a8349aa241a9aa45b1fbf0aa7294ac8768cc30926cc9f2e7e4eca3007eb2dfe0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a8349aa241a9aa45b1fbf0aa7294ac8768cc30926cc9f2e7e4eca3007eb2dfe0","first_computed_at":"2026-05-18T01:30:49.539007Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:30:49.539007Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XgTd8osAsUQfjfEqjb0IWX4WxoibtJz7EBPAO/nf01ZMcCaDkRDHAPlEzRXhpEJB7tEziNpj0dlcJxHFXlFuCg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:30:49.539534Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.5943","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bedd1ffac2c6337cd4a1c8e5098bde93ba4c9c32da98a1b93192c802a3248ac9","sha256:b2153f44b2e3013ff4ff1b2d8f52480fa40ab4ccd8228cc3c726c9092a7c3180"],"state_sha256":"1a10b6d4a59f68ce295c8190393ffbaa495b9dfc45e0350e7bf54260eb3a798a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P3slFoxs4NkCZoMwoIw6D1QCySB9zxi5WbtW9oTHFi/2IiVvF3D3vN6xYtYWZ+lCOeO2I26VUD8wYEFDqhk8Ag==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T10:51:31.381563Z","bundle_sha256":"f63f4a4be68805bc919744e2fea1cb5a62e08acaef35ea5620a8b0c8fd05e866"}}