{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:FTVEJB2MMIQBJJAECFJ2OXPGXB","short_pith_number":"pith:FTVEJB2M","canonical_record":{"source":{"id":"1407.2372","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-09T07:26:04Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"aeba576a069eaa700ae9dbde467586574382c098937088626ff0f3e1107fd0e9","abstract_canon_sha256":"d009d53c41b92d4f0e6d2fb6540c1ba7c8ffd3897e90f2caa6d770fc726181da"},"schema_version":"1.0"},"canonical_sha256":"2cea44874c622014a4041153a75de6b86d2e3e3c01818c032afa8c1d1573227a","source":{"kind":"arxiv","id":"1407.2372","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2372","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2372v4","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2372","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"pith_short_12","alias_value":"FTVEJB2MMIQB","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FTVEJB2MMIQBJJAE","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FTVEJB2M","created_at":"2026-05-18T12:28:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:FTVEJB2MMIQBJJAECFJ2OXPGXB","target":"record","payload":{"canonical_record":{"source":{"id":"1407.2372","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-09T07:26:04Z","cross_cats_sorted":["hep-lat","nucl-th"],"title_canon_sha256":"aeba576a069eaa700ae9dbde467586574382c098937088626ff0f3e1107fd0e9","abstract_canon_sha256":"d009d53c41b92d4f0e6d2fb6540c1ba7c8ffd3897e90f2caa6d770fc726181da"},"schema_version":"1.0"},"canonical_sha256":"2cea44874c622014a4041153a75de6b86d2e3e3c01818c032afa8c1d1573227a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:38.723924Z","signature_b64":"jIFTycAhyNfTFTZc7362LfV7MzidhXGML0aBYwJZn4nNzPWj3YAcpN1b/eA4iUpUzjTlydBiBY4S09zdDjZoBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2cea44874c622014a4041153a75de6b86d2e3e3c01818c032afa8c1d1573227a","last_reissued_at":"2026-05-18T01:42:38.723219Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:38.723219Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1407.2372","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:42:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tm7Hh6STHZx+QUIFjnkPSm3O7mIR7hMs/eAw+VqOWW5Y//YcsobScGDdHUnSVL6KmaqlTMI20beS/lqLuPDRBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:02:41.693549Z"},"content_sha256":"2de518ef6b05218d0ce3364c9a48cab07ab1dfd3f3e2613a2c07326ab46e7076","schema_version":"1.0","event_id":"sha256:2de518ef6b05218d0ce3364c9a48cab07ab1dfd3f3e2613a2c07326ab46e7076"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:FTVEJB2MMIQBJJAECFJ2OXPGXB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hadron mass scaling near the s-wave threshold","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Tetsuo Hyodo","submitted_at":"2014-07-09T07:26:04Z","abstract_excerpt":"The influence of a two-hadron threshold is studied for the hadron mass scaling with respect to some quantum chromodynamics parameters. A quantum mechanical model is introduced to describe the system with a one-body bare state coupled with a single elastic two-body scattering. The general behavior of the energy of the bound and resonance state near the two-body threshold for a local potential is derived from the expansion of the Jost function around the threshold. It is shown that the same scaling holds for the nonlocal potential induced by the coupling to a bare state. In p or higher partial w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2372","kind":"arxiv","version":4},"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":"2026-05-18T01:42:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8kYpAhY2z5LtImpwMGlyINNPYac7orME/5gBlLUMKnzXh5DuddKtI3oO2dzZhM3JxWRfSF8Bmm67fAE0K7HFDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T23:02:41.693898Z"},"content_sha256":"e2795208cdc3dd844f73f165da58833fd87a9695ed17d42e53e882b380705521","schema_version":"1.0","event_id":"sha256:e2795208cdc3dd844f73f165da58833fd87a9695ed17d42e53e882b380705521"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/bundle.json","state_url":"https://pith.science/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/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":"2026-06-01T23:02:41Z","links":{"resolver":"https://pith.science/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB","bundle":"https://pith.science/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/bundle.json","state":"https://pith.science/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FTVEJB2MMIQBJJAECFJ2OXPGXB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:FTVEJB2MMIQBJJAECFJ2OXPGXB","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":"d009d53c41b92d4f0e6d2fb6540c1ba7c8ffd3897e90f2caa6d770fc726181da","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-09T07:26:04Z","title_canon_sha256":"aeba576a069eaa700ae9dbde467586574382c098937088626ff0f3e1107fd0e9"},"schema_version":"1.0","source":{"id":"1407.2372","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.2372","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"arxiv_version","alias_value":"1407.2372v4","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.2372","created_at":"2026-05-18T01:42:38Z"},{"alias_kind":"pith_short_12","alias_value":"FTVEJB2MMIQB","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_16","alias_value":"FTVEJB2MMIQBJJAE","created_at":"2026-05-18T12:28:28Z"},{"alias_kind":"pith_short_8","alias_value":"FTVEJB2M","created_at":"2026-05-18T12:28:28Z"}],"graph_snapshots":[{"event_id":"sha256:e2795208cdc3dd844f73f165da58833fd87a9695ed17d42e53e882b380705521","target":"graph","created_at":"2026-05-18T01:42:38Z","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":"The influence of a two-hadron threshold is studied for the hadron mass scaling with respect to some quantum chromodynamics parameters. A quantum mechanical model is introduced to describe the system with a one-body bare state coupled with a single elastic two-body scattering. The general behavior of the energy of the bound and resonance state near the two-body threshold for a local potential is derived from the expansion of the Jost function around the threshold. It is shown that the same scaling holds for the nonlocal potential induced by the coupling to a bare state. In p or higher partial w","authors_text":"Tetsuo Hyodo","cross_cats":["hep-lat","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-09T07:26:04Z","title":"Hadron mass scaling near the s-wave threshold"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.2372","kind":"arxiv","version":4},"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":"sha256:2de518ef6b05218d0ce3364c9a48cab07ab1dfd3f3e2613a2c07326ab46e7076","target":"record","created_at":"2026-05-18T01:42:38Z","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":"d009d53c41b92d4f0e6d2fb6540c1ba7c8ffd3897e90f2caa6d770fc726181da","cross_cats_sorted":["hep-lat","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-07-09T07:26:04Z","title_canon_sha256":"aeba576a069eaa700ae9dbde467586574382c098937088626ff0f3e1107fd0e9"},"schema_version":"1.0","source":{"id":"1407.2372","kind":"arxiv","version":4}},"canonical_sha256":"2cea44874c622014a4041153a75de6b86d2e3e3c01818c032afa8c1d1573227a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2cea44874c622014a4041153a75de6b86d2e3e3c01818c032afa8c1d1573227a","first_computed_at":"2026-05-18T01:42:38.723219Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:42:38.723219Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jIFTycAhyNfTFTZc7362LfV7MzidhXGML0aBYwJZn4nNzPWj3YAcpN1b/eA4iUpUzjTlydBiBY4S09zdDjZoBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:42:38.723924Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.2372","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2de518ef6b05218d0ce3364c9a48cab07ab1dfd3f3e2613a2c07326ab46e7076","sha256:e2795208cdc3dd844f73f165da58833fd87a9695ed17d42e53e882b380705521"],"state_sha256":"fb62d13f582547176ad662bb23c70fd0e65ffc52abab2e0890026cdb66d0a6df"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"42byO9Zmf9TjWqTTAI5VieVMZ7KHGZ3NKXnhCdU5HjmKlVKH//Zys/b54pTdXG1V5NH4/97iMRUTvgOc4GN0CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T23:02:41.695858Z","bundle_sha256":"73825967170552556d106802ff31bc35929adbbcdb559c509b0d9839eae10f14"}}