{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:55ITKLFOWRYSU666DEPKUOT5EZ","short_pith_number":"pith:55ITKLFO","canonical_record":{"source":{"id":"1505.05415","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-05-20T15:19:12Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"12219d1e3e3c394c9823ec40942ee6d13897a96890f141cfcd99606793a8c857","abstract_canon_sha256":"7b49ac3448d1d1881f0201cd43680c89a296d60e59371bf484041d1ac0c06e36"},"schema_version":"1.0"},"canonical_sha256":"ef51352caeb4712a7bde191eaa3a7d2677bf384222fd06f8c8ce84085fa47a36","source":{"kind":"arxiv","id":"1505.05415","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.05415","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"arxiv_version","alias_value":"1505.05415v2","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05415","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"pith_short_12","alias_value":"55ITKLFOWRYS","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"55ITKLFOWRYSU666","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"55ITKLFO","created_at":"2026-05-18T12:29:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:55ITKLFOWRYSU666DEPKUOT5EZ","target":"record","payload":{"canonical_record":{"source":{"id":"1505.05415","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-05-20T15:19:12Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"12219d1e3e3c394c9823ec40942ee6d13897a96890f141cfcd99606793a8c857","abstract_canon_sha256":"7b49ac3448d1d1881f0201cd43680c89a296d60e59371bf484041d1ac0c06e36"},"schema_version":"1.0"},"canonical_sha256":"ef51352caeb4712a7bde191eaa3a7d2677bf384222fd06f8c8ce84085fa47a36","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:55.862639Z","signature_b64":"iukrF9HmdpaRiTS67GLd8DJbQs6L2i2pGurvLvn2epN1IopLk/vrdBaJsRJICGvOf2SW/tDUNyMxJsIPYek4Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef51352caeb4712a7bde191eaa3a7d2677bf384222fd06f8c8ce84085fa47a36","last_reissued_at":"2026-05-18T01:28:55.861871Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:55.861871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1505.05415","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":"2026-05-18T01:28:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9Rg81QhI+A/YtlfxWqtSKc9OKOiWQAGJ9Nb9E5IQ4OOwtQXgOoVR7VQkQX3Ks9gmg4CsKuptTOMggDQOOA4GAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T19:39:36.586491Z"},"content_sha256":"d983fb30eda221b99d4fd48f10eaabb362b698445e2d33c11aa2a5c3ef67dddf","schema_version":"1.0","event_id":"sha256:d983fb30eda221b99d4fd48f10eaabb362b698445e2d33c11aa2a5c3ef67dddf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:55ITKLFOWRYSU666DEPKUOT5EZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling violation and relativistic effective mass from quasielastic electron scattering: implications for neutrino reactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"E. Ruiz Arriola, I. Ruiz Simo, J.E. Amaro","submitted_at":"2015-05-20T15:19:12Z","abstract_excerpt":"The experimental data from quasielastic electron scattering from $^{12}$C are reanalyzed in terms of a new scaling variable suggested by the interacting relativistic Fermi gas with scalar and vector interactions, which is known to generate a relativistic effective mass for the interacting nucleons. By choosing a mean value of this relativistic effective mass $m_N^* =0.8 m_N$, we observe that most of the data fall inside a region around the inverse parabola-shaped universal scaling function of the relativistic Fermi gas. This suggests a method to select the subset of data that highlight the qua"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05415","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":"2026-05-18T01:28:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Uj1PQz/9Z41CEwnbF98AcYMMksYTwi076/RnTIhjyTuza2hQ9UbFQD4b2h4xy+EmDi8UgR3gpbT9XqAHqITECw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T19:39:36.586831Z"},"content_sha256":"9c94e74e0de81e916766d302523954fa40320302b50e494b609794e70f0086c7","schema_version":"1.0","event_id":"sha256:9c94e74e0de81e916766d302523954fa40320302b50e494b609794e70f0086c7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/55ITKLFOWRYSU666DEPKUOT5EZ/bundle.json","state_url":"https://pith.science/pith/55ITKLFOWRYSU666DEPKUOT5EZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/55ITKLFOWRYSU666DEPKUOT5EZ/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":"2026-06-01T19:39:36Z","links":{"resolver":"https://pith.science/pith/55ITKLFOWRYSU666DEPKUOT5EZ","bundle":"https://pith.science/pith/55ITKLFOWRYSU666DEPKUOT5EZ/bundle.json","state":"https://pith.science/pith/55ITKLFOWRYSU666DEPKUOT5EZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/55ITKLFOWRYSU666DEPKUOT5EZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:55ITKLFOWRYSU666DEPKUOT5EZ","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":"7b49ac3448d1d1881f0201cd43680c89a296d60e59371bf484041d1ac0c06e36","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-05-20T15:19:12Z","title_canon_sha256":"12219d1e3e3c394c9823ec40942ee6d13897a96890f141cfcd99606793a8c857"},"schema_version":"1.0","source":{"id":"1505.05415","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1505.05415","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"arxiv_version","alias_value":"1505.05415v2","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.05415","created_at":"2026-05-18T01:28:55Z"},{"alias_kind":"pith_short_12","alias_value":"55ITKLFOWRYS","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"55ITKLFOWRYSU666","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"55ITKLFO","created_at":"2026-05-18T12:29:05Z"}],"graph_snapshots":[{"event_id":"sha256:9c94e74e0de81e916766d302523954fa40320302b50e494b609794e70f0086c7","target":"graph","created_at":"2026-05-18T01:28:55Z","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 experimental data from quasielastic electron scattering from $^{12}$C are reanalyzed in terms of a new scaling variable suggested by the interacting relativistic Fermi gas with scalar and vector interactions, which is known to generate a relativistic effective mass for the interacting nucleons. By choosing a mean value of this relativistic effective mass $m_N^* =0.8 m_N$, we observe that most of the data fall inside a region around the inverse parabola-shaped universal scaling function of the relativistic Fermi gas. This suggests a method to select the subset of data that highlight the qua","authors_text":"E. Ruiz Arriola, I. Ruiz Simo, J.E. Amaro","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-05-20T15:19:12Z","title":"Scaling violation and relativistic effective mass from quasielastic electron scattering: implications for neutrino reactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.05415","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:d983fb30eda221b99d4fd48f10eaabb362b698445e2d33c11aa2a5c3ef67dddf","target":"record","created_at":"2026-05-18T01:28:55Z","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":"7b49ac3448d1d1881f0201cd43680c89a296d60e59371bf484041d1ac0c06e36","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-05-20T15:19:12Z","title_canon_sha256":"12219d1e3e3c394c9823ec40942ee6d13897a96890f141cfcd99606793a8c857"},"schema_version":"1.0","source":{"id":"1505.05415","kind":"arxiv","version":2}},"canonical_sha256":"ef51352caeb4712a7bde191eaa3a7d2677bf384222fd06f8c8ce84085fa47a36","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef51352caeb4712a7bde191eaa3a7d2677bf384222fd06f8c8ce84085fa47a36","first_computed_at":"2026-05-18T01:28:55.861871Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:28:55.861871Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iukrF9HmdpaRiTS67GLd8DJbQs6L2i2pGurvLvn2epN1IopLk/vrdBaJsRJICGvOf2SW/tDUNyMxJsIPYek4Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:28:55.862639Z","signed_message":"canonical_sha256_bytes"},"source_id":"1505.05415","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d983fb30eda221b99d4fd48f10eaabb362b698445e2d33c11aa2a5c3ef67dddf","sha256:9c94e74e0de81e916766d302523954fa40320302b50e494b609794e70f0086c7"],"state_sha256":"302e4eed4d543910c27535fd3445633bbfaa8d057a589cad045ac874d66315f9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QHRJxkuZqiIJYsLsyzhvCoZtfsdshslh2Ml2fod76dSgB/lqAQnYuBOnrRQ+fBwhI8qPTuy5k07l2PYdQNK/BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T19:39:36.588763Z","bundle_sha256":"f0d382e84b527bf76db7d274cf2e6fb8af8fbba98ba272ca6981103b3b4245d4"}}