{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:TVETXNPXL2U6HEBOA3HGKWHZJF","short_pith_number":"pith:TVETXNPX","canonical_record":{"source":{"id":"1002.4924","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-02-26T05:26:56Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"8f081807a8845705306f5c835c38941608ae90d6dd4a79881dfc78c745d44224","abstract_canon_sha256":"4da3012837d896b522a1d09a529eed7386370ff383c65522f55ec2aa889cb2d3"},"schema_version":"1.0"},"canonical_sha256":"9d493bb5f75ea9e3902e06ce6558f94949b1ed4c532718999deaaac0bc523db8","source":{"kind":"arxiv","id":"1002.4924","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.4924","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"arxiv_version","alias_value":"1002.4924v3","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.4924","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"pith_short_12","alias_value":"TVETXNPXL2U6","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"TVETXNPXL2U6HEBO","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"TVETXNPX","created_at":"2026-05-18T12:26:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:TVETXNPXL2U6HEBOA3HGKWHZJF","target":"record","payload":{"canonical_record":{"source":{"id":"1002.4924","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-02-26T05:26:56Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"8f081807a8845705306f5c835c38941608ae90d6dd4a79881dfc78c745d44224","abstract_canon_sha256":"4da3012837d896b522a1d09a529eed7386370ff383c65522f55ec2aa889cb2d3"},"schema_version":"1.0"},"canonical_sha256":"9d493bb5f75ea9e3902e06ce6558f94949b1ed4c532718999deaaac0bc523db8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:24:38.494064Z","signature_b64":"wv8ygCGL83eq+T/egkojPEDUaSHfonhGyJE9gi7vpv/T8N9o/I9RDvs7rlgs9plID7WFFSf3PebK44lHeJamCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d493bb5f75ea9e3902e06ce6558f94949b1ed4c532718999deaaac0bc523db8","last_reissued_at":"2026-05-18T02:24:38.493531Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:24:38.493531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1002.4924","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:24:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OTEKS8mueZAnoDubagsuXdnh+X1te8yBk6WLvUYxjqdWJZPFsdTeOmC3YwR1rSn6a/fmWfvBdCujreuXoCnWAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:15:57.286393Z"},"content_sha256":"69763020c4d9dbb1c73ed8a52cb0cc9981935e40412a4963a6141021bdbaab11","schema_version":"1.0","event_id":"sha256:69763020c4d9dbb1c73ed8a52cb0cc9981935e40412a4963a6141021bdbaab11"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:TVETXNPXL2U6HEBOA3HGKWHZJF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Power Counting Regime of Chiral Effective Field Theory and Beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"D. B. Leinweber, J. M. M. Hall, R. D. Young","submitted_at":"2010-02-26T05:26:56Z","abstract_excerpt":"Chiral effective field theory complements numerical simulations of quantum chromodynamics (QCD) on a space-time lattice. It provides a model-independent formalism for connecting lattice simulation results at finite volume and a variety of quark masses to the physical world. The asymptotic nature of the chiral expansion places the focus on the first few terms of the expansion. Thus, knowledge of the power-counting regime (PCR) of chiral effective field theory, where higher-order terms of the expansion may be regarded as negligible, is as important as knowledge of the expansion itself. Through t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.4924","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:24:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QopUifqSjN5/4TpGHilYc4HsSqVMvlzQ/u4cRYR50DfMGxn9VVLoM2/f21E3v4eK6bpZWPHrAtqT30qLC++IDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T01:15:57.286751Z"},"content_sha256":"66bbcd97127c23a1d08287aa64b4dfe9cc8b025d28af86da613a4c91294b994f","schema_version":"1.0","event_id":"sha256:66bbcd97127c23a1d08287aa64b4dfe9cc8b025d28af86da613a4c91294b994f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/bundle.json","state_url":"https://pith.science/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/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":"2026-05-28T01:15:57Z","links":{"resolver":"https://pith.science/pith/TVETXNPXL2U6HEBOA3HGKWHZJF","bundle":"https://pith.science/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/bundle.json","state":"https://pith.science/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TVETXNPXL2U6HEBOA3HGKWHZJF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:TVETXNPXL2U6HEBOA3HGKWHZJF","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":"4da3012837d896b522a1d09a529eed7386370ff383c65522f55ec2aa889cb2d3","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-02-26T05:26:56Z","title_canon_sha256":"8f081807a8845705306f5c835c38941608ae90d6dd4a79881dfc78c745d44224"},"schema_version":"1.0","source":{"id":"1002.4924","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1002.4924","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"arxiv_version","alias_value":"1002.4924v3","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1002.4924","created_at":"2026-05-18T02:24:38Z"},{"alias_kind":"pith_short_12","alias_value":"TVETXNPXL2U6","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"TVETXNPXL2U6HEBO","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"TVETXNPX","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:66bbcd97127c23a1d08287aa64b4dfe9cc8b025d28af86da613a4c91294b994f","target":"graph","created_at":"2026-05-18T02:24:38Z","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":"Chiral effective field theory complements numerical simulations of quantum chromodynamics (QCD) on a space-time lattice. It provides a model-independent formalism for connecting lattice simulation results at finite volume and a variety of quark masses to the physical world. The asymptotic nature of the chiral expansion places the focus on the first few terms of the expansion. Thus, knowledge of the power-counting regime (PCR) of chiral effective field theory, where higher-order terms of the expansion may be regarded as negligible, is as important as knowledge of the expansion itself. Through t","authors_text":"D. B. Leinweber, J. M. M. Hall, R. D. Young","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-02-26T05:26:56Z","title":"Power Counting Regime of Chiral Effective Field Theory and Beyond"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1002.4924","kind":"arxiv","version":3},"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":"sha256:69763020c4d9dbb1c73ed8a52cb0cc9981935e40412a4963a6141021bdbaab11","target":"record","created_at":"2026-05-18T02:24:38Z","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":"4da3012837d896b522a1d09a529eed7386370ff383c65522f55ec2aa889cb2d3","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2010-02-26T05:26:56Z","title_canon_sha256":"8f081807a8845705306f5c835c38941608ae90d6dd4a79881dfc78c745d44224"},"schema_version":"1.0","source":{"id":"1002.4924","kind":"arxiv","version":3}},"canonical_sha256":"9d493bb5f75ea9e3902e06ce6558f94949b1ed4c532718999deaaac0bc523db8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9d493bb5f75ea9e3902e06ce6558f94949b1ed4c532718999deaaac0bc523db8","first_computed_at":"2026-05-18T02:24:38.493531Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:24:38.493531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wv8ygCGL83eq+T/egkojPEDUaSHfonhGyJE9gi7vpv/T8N9o/I9RDvs7rlgs9plID7WFFSf3PebK44lHeJamCA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:24:38.494064Z","signed_message":"canonical_sha256_bytes"},"source_id":"1002.4924","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:69763020c4d9dbb1c73ed8a52cb0cc9981935e40412a4963a6141021bdbaab11","sha256:66bbcd97127c23a1d08287aa64b4dfe9cc8b025d28af86da613a4c91294b994f"],"state_sha256":"1726ffec0d9bde9665c03cd798c8484b1cfb8a357f527202f3a24df9b4705ff2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RK9vt586EJigETg01G5Ya347NnchTJnY29HTlMw0S88U+4V5wtO6MnwsHEBzHFBdWPPvDsOgZ9LcgWPP0DysAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T01:15:57.288938Z","bundle_sha256":"1345705c9d915dc14487332d4a8df93e239084240836cc76044a5b05a3e3809e"}}