{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:5AISKOJDTDARGGQFJQG2XUQKP3","short_pith_number":"pith:5AISKOJD","canonical_record":{"source":{"id":"1902.01295","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-04T16:40:51Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"9b1442656531b1bb7081c3e0b9b8ffd060a389705420d03c576f0ed764532e7a","abstract_canon_sha256":"6de2d385aa57391abc23aeaacee5388100e3de3b6c9b7a85e794ee89d5c32013"},"schema_version":"1.0"},"canonical_sha256":"e81125392398c1131a054c0dabd20a7ec01e45455281cb910b969b9e929744fe","source":{"kind":"arxiv","id":"1902.01295","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.01295","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"arxiv_version","alias_value":"1902.01295v1","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.01295","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"pith_short_12","alias_value":"5AISKOJDTDAR","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"5AISKOJDTDARGGQF","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"5AISKOJD","created_at":"2026-05-18T12:33:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:5AISKOJDTDARGGQFJQG2XUQKP3","target":"record","payload":{"canonical_record":{"source":{"id":"1902.01295","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-04T16:40:51Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"9b1442656531b1bb7081c3e0b9b8ffd060a389705420d03c576f0ed764532e7a","abstract_canon_sha256":"6de2d385aa57391abc23aeaacee5388100e3de3b6c9b7a85e794ee89d5c32013"},"schema_version":"1.0"},"canonical_sha256":"e81125392398c1131a054c0dabd20a7ec01e45455281cb910b969b9e929744fe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:41:45.162402Z","signature_b64":"8XZ5pa18dI5xeGPX8/LUcbsAZmnP4bwyI6/WiM2hqgR0YvsKp0MCgYv03Y3KfVxXHGwgYtCXD7hPVDN4ixYpDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e81125392398c1131a054c0dabd20a7ec01e45455281cb910b969b9e929744fe","last_reissued_at":"2026-05-17T23:41:45.161926Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:41:45.161926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1902.01295","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:41:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9OUUfdJJu8ioiFntk2aiLmv8gbC+ytKxSIfO23kJ1akuCEXvbOQRzd4ACd4vehrdiVRrM+GzXcHaWJAXRTtlAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:13:55.021410Z"},"content_sha256":"2ac576e59ebbea0f117648fa35ef7ca7bacaf78dc4b314293922f4c2e72978eb","schema_version":"1.0","event_id":"sha256:2ac576e59ebbea0f117648fa35ef7ca7bacaf78dc4b314293922f4c2e72978eb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:5AISKOJDTDARGGQFJQG2XUQKP3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Galilean invariance restoration on the lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"nucl-th","authors_text":"Bing-Nan Lu, Dean Lee, Evgeny Epelbaum, Ning Li, Serdar Elhatisari, Ulf-G. Mei{\\ss}ner","submitted_at":"2019-02-04T16:40:51Z","abstract_excerpt":"We consider the breaking of Galilean invariance due to different lattice cutoff effects in moving frames and a nonlocal smearing parameter which is used in the construction of the nuclear lattice interaction. The dispersion relation and neutron-proton scattering phase shifts are used to investigate the Galilean invariance breaking effects and ways to restore it. For $S$-wave channels, ${}^1S_0$ and ${}^3S_1$, we present the neutron-proton scattering phase shifts in moving frames calculated using both L\\\"uscher's formula and the spherical wall method, as well as the dispersion relation. For the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.01295","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":""},"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":"2026-05-17T23:41:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3b/DRll6i1mawOrYdDVacQQvWjTbvWQnQbbd5oB2yyQLiCgLl/sXKpvwlvHqeW9igmrR++tlaW4WB85NhKcQCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T13:13:55.021932Z"},"content_sha256":"670020ccd0a575fecd0c248b59fbdc8165611a0a63e32f08a902f370c371b269","schema_version":"1.0","event_id":"sha256:670020ccd0a575fecd0c248b59fbdc8165611a0a63e32f08a902f370c371b269"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5AISKOJDTDARGGQFJQG2XUQKP3/bundle.json","state_url":"https://pith.science/pith/5AISKOJDTDARGGQFJQG2XUQKP3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5AISKOJDTDARGGQFJQG2XUQKP3/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":"2026-05-27T13:13:55Z","links":{"resolver":"https://pith.science/pith/5AISKOJDTDARGGQFJQG2XUQKP3","bundle":"https://pith.science/pith/5AISKOJDTDARGGQFJQG2XUQKP3/bundle.json","state":"https://pith.science/pith/5AISKOJDTDARGGQFJQG2XUQKP3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5AISKOJDTDARGGQFJQG2XUQKP3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:5AISKOJDTDARGGQFJQG2XUQKP3","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":"6de2d385aa57391abc23aeaacee5388100e3de3b6c9b7a85e794ee89d5c32013","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-04T16:40:51Z","title_canon_sha256":"9b1442656531b1bb7081c3e0b9b8ffd060a389705420d03c576f0ed764532e7a"},"schema_version":"1.0","source":{"id":"1902.01295","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.01295","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"arxiv_version","alias_value":"1902.01295v1","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.01295","created_at":"2026-05-17T23:41:45Z"},{"alias_kind":"pith_short_12","alias_value":"5AISKOJDTDAR","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_16","alias_value":"5AISKOJDTDARGGQF","created_at":"2026-05-18T12:33:10Z"},{"alias_kind":"pith_short_8","alias_value":"5AISKOJD","created_at":"2026-05-18T12:33:10Z"}],"graph_snapshots":[{"event_id":"sha256:670020ccd0a575fecd0c248b59fbdc8165611a0a63e32f08a902f370c371b269","target":"graph","created_at":"2026-05-17T23:41:45Z","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 consider the breaking of Galilean invariance due to different lattice cutoff effects in moving frames and a nonlocal smearing parameter which is used in the construction of the nuclear lattice interaction. The dispersion relation and neutron-proton scattering phase shifts are used to investigate the Galilean invariance breaking effects and ways to restore it. For $S$-wave channels, ${}^1S_0$ and ${}^3S_1$, we present the neutron-proton scattering phase shifts in moving frames calculated using both L\\\"uscher's formula and the spherical wall method, as well as the dispersion relation. For the","authors_text":"Bing-Nan Lu, Dean Lee, Evgeny Epelbaum, Ning Li, Serdar Elhatisari, Ulf-G. Mei{\\ss}ner","cross_cats":["hep-lat"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-04T16:40:51Z","title":"Galilean invariance restoration on the lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.01295","kind":"arxiv","version":1},"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":"sha256:2ac576e59ebbea0f117648fa35ef7ca7bacaf78dc4b314293922f4c2e72978eb","target":"record","created_at":"2026-05-17T23:41:45Z","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":"6de2d385aa57391abc23aeaacee5388100e3de3b6c9b7a85e794ee89d5c32013","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-04T16:40:51Z","title_canon_sha256":"9b1442656531b1bb7081c3e0b9b8ffd060a389705420d03c576f0ed764532e7a"},"schema_version":"1.0","source":{"id":"1902.01295","kind":"arxiv","version":1}},"canonical_sha256":"e81125392398c1131a054c0dabd20a7ec01e45455281cb910b969b9e929744fe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e81125392398c1131a054c0dabd20a7ec01e45455281cb910b969b9e929744fe","first_computed_at":"2026-05-17T23:41:45.161926Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:41:45.161926Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8XZ5pa18dI5xeGPX8/LUcbsAZmnP4bwyI6/WiM2hqgR0YvsKp0MCgYv03Y3KfVxXHGwgYtCXD7hPVDN4ixYpDQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:41:45.162402Z","signed_message":"canonical_sha256_bytes"},"source_id":"1902.01295","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2ac576e59ebbea0f117648fa35ef7ca7bacaf78dc4b314293922f4c2e72978eb","sha256:670020ccd0a575fecd0c248b59fbdc8165611a0a63e32f08a902f370c371b269"],"state_sha256":"bed8328bb720034fec4cdcea0e098cd476f8c7241835e9f20f598797722c6ea0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0gjorcySqTyCMg5e6k58RUXDSLusSf+W758f8v5dK0yqIgOsfpJ+NkTBvrlMDzANbwi9PUBa9y8KAFrl8HzlDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T13:13:55.024206Z","bundle_sha256":"d6f058aad98d6f01f91a261e431757080cc8d11e3a0f792a8dd3fc4815a26465"}}