{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:MQQCHQ2QQF7RWUNTOLUAKNSM2Z","short_pith_number":"pith:MQQCHQ2Q","schema_version":"1.0","canonical_sha256":"642023c350817f1b51b372e805364cd65734da17512e303819b84c42829cf943","source":{"kind":"arxiv","id":"hep-lat/0509133","version":1},"attestation_state":"computed","paper":{"title":"Structure of the Pion from Full Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Sch\\\"afer, D. Br\\\"ommel, D. Pleiter, G. Schierholz, J.M. Zanotti (QCDSF/UKQCD Collaboration), M. Diehl, M. G\\\"ockeler, P.E.L. Rakow, Ph. H\\\"agler, R. Horsley","submitted_at":"2005-09-26T17:01:06Z","abstract_excerpt":"Moments of generalised parton distributions can be related to off-forward matrix elements of local operators. We calculate a few of the leading twist matrix elements for the pion on the lattice. The simulations are performed using two flavours of dynamical fermions and a range of pion masses from 550 to 1090 MeV. Our lattice spacings and spatial volumes lie in the range 0.07-0.12 fm and (1.6-2.2 fm)^3, respectively. Key features of our investigation are the use of O(a) improved Wilson fermions and non-perturbative renormalisation. We present first results for the two lowest moments of the gene"},"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":"hep-lat/0509133","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-09-26T17:01:06Z","cross_cats_sorted":[],"title_canon_sha256":"95e5fff22cac93e516e754e5200740ba464afc5aa1bcd44fd262161a34ca59d7","abstract_canon_sha256":"e671a73ff54a0fe3b2315da873c010e104247fbf5f64dd8b4a458b62f4395c73"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:28:47.331773Z","signature_b64":"vxuSRqWYP5LZlsiYNKrSzmmTuZ2UkQZOrXQnpGzWJOMONwwjMAzKOmgwh1u6DIhYEAqU3OuTxCJI6cWWkt96BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"642023c350817f1b51b372e805364cd65734da17512e303819b84c42829cf943","last_reissued_at":"2026-07-04T15:28:47.331324Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:28:47.331324Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Structure of the Pion from Full Lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Sch\\\"afer, D. Br\\\"ommel, D. Pleiter, G. Schierholz, J.M. Zanotti (QCDSF/UKQCD Collaboration), M. Diehl, M. G\\\"ockeler, P.E.L. Rakow, Ph. H\\\"agler, R. Horsley","submitted_at":"2005-09-26T17:01:06Z","abstract_excerpt":"Moments of generalised parton distributions can be related to off-forward matrix elements of local operators. We calculate a few of the leading twist matrix elements for the pion on the lattice. The simulations are performed using two flavours of dynamical fermions and a range of pion masses from 550 to 1090 MeV. Our lattice spacings and spatial volumes lie in the range 0.07-0.12 fm and (1.6-2.2 fm)^3, respectively. Key features of our investigation are the use of O(a) improved Wilson fermions and non-perturbative renormalisation. We present first results for the two lowest moments of the gene"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0509133","kind":"arxiv","version":1},"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/hep-lat/0509133/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":"hep-lat/0509133","created_at":"2026-07-04T15:28:47.331388+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0509133v1","created_at":"2026-07-04T15:28:47.331388+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0509133","created_at":"2026-07-04T15:28:47.331388+00:00"},{"alias_kind":"pith_short_12","alias_value":"MQQCHQ2QQF7R","created_at":"2026-07-04T15:28:47.331388+00:00"},{"alias_kind":"pith_short_16","alias_value":"MQQCHQ2QQF7RWUNT","created_at":"2026-07-04T15:28:47.331388+00:00"},{"alias_kind":"pith_short_8","alias_value":"MQQCHQ2Q","created_at":"2026-07-04T15:28:47.331388+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/MQQCHQ2QQF7RWUNTOLUAKNSM2Z","json":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z.json","graph_json":"https://pith.science/api/pith-number/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/graph.json","events_json":"https://pith.science/api/pith-number/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/events.json","paper":"https://pith.science/paper/MQQCHQ2Q"},"agent_actions":{"view_html":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z","download_json":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z.json","view_paper":"https://pith.science/paper/MQQCHQ2Q","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0509133&json=true","fetch_graph":"https://pith.science/api/pith-number/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/graph.json","fetch_events":"https://pith.science/api/pith-number/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/action/storage_attestation","attest_author":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/action/author_attestation","sign_citation":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/action/citation_signature","submit_replication":"https://pith.science/pith/MQQCHQ2QQF7RWUNTOLUAKNSM2Z/action/replication_record"}},"created_at":"2026-07-04T15:28:47.331388+00:00","updated_at":"2026-07-04T15:28:47.331388+00:00"}