{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:M2RM62M7G7UUL7V3ZWUPHVBGX5","short_pith_number":"pith:M2RM62M7","canonical_record":{"source":{"id":"1804.07548","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-20T11:02:48Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"79886cbec5b10c43beb9ee0c8e9cd9f53593ef7e136aa52bbe32b5d2066bb1a7","abstract_canon_sha256":"33d5dedfeeb570b7f871e9dfef91cf159a377ee91f1efc533887d2dc76b3d8d4"},"schema_version":"1.0"},"canonical_sha256":"66a2cf699f37e945febbcda8f3d426bf5ed4b38789c09027d213da3fc77241ac","source":{"kind":"arxiv","id":"1804.07548","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.07548","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"arxiv_version","alias_value":"1804.07548v1","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.07548","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"pith_short_12","alias_value":"M2RM62M7G7UU","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"M2RM62M7G7UUL7V3","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"M2RM62M7","created_at":"2026-05-18T12:32:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:M2RM62M7G7UUL7V3ZWUPHVBGX5","target":"record","payload":{"canonical_record":{"source":{"id":"1804.07548","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-20T11:02:48Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"79886cbec5b10c43beb9ee0c8e9cd9f53593ef7e136aa52bbe32b5d2066bb1a7","abstract_canon_sha256":"33d5dedfeeb570b7f871e9dfef91cf159a377ee91f1efc533887d2dc76b3d8d4"},"schema_version":"1.0"},"canonical_sha256":"66a2cf699f37e945febbcda8f3d426bf5ed4b38789c09027d213da3fc77241ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:13:26.105959Z","signature_b64":"RhePmbQfh2fl7UTHsVusFj2oywcMWZeqg5hNHc21m4anVo5dLbiUIBr02GFWy3a+YUURkOqn1XB2Mr/fqs8ICg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66a2cf699f37e945febbcda8f3d426bf5ed4b38789c09027d213da3fc77241ac","last_reissued_at":"2026-05-18T00:13:26.105281Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:13:26.105281Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1804.07548","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":"2026-05-18T00:13:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3b4ObYjzc4wbW7uh+GHeKLuyBjMun1LBnp5rLQiJqUE1BEil/tbN5b1ukcIPT7Fgm/8yiCLee/dJWZw6CaI3Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T06:09:02.118052Z"},"content_sha256":"e4f3de4db4399b32423da9243aeb15987bcf41fde029fd112c93d1a2e0d0309e","schema_version":"1.0","event_id":"sha256:e4f3de4db4399b32423da9243aeb15987bcf41fde029fd112c93d1a2e0d0309e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:M2RM62M7G7UUL7V3ZWUPHVBGX5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quasielastic charged-current neutrino scattering in the scaling model with relativistic effective mass","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, V.L. Martinez-Consentino","submitted_at":"2018-04-20T11:02:48Z","abstract_excerpt":"We use a recent scaling analysis of the quasielastic electron scattering data from $^{12}$C to predict the quasielastic charge-changing neutrino scattering cross sections within an uncertainty band. We use a scaling function extracted from a selection of the $(e,e')$ cross section data, and an effective nucleon mass inspired by the relativistic mean-field model of nuclear matter. The corresponding super-scaling analysis with relativistic effective mass (SuSAM*) describes a large amount of the electron data lying inside a phenomenological quasielastic band. The effective mass incorporates the e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.07548","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":"2026-05-18T00:13:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nxQXNLqnbOObKshTKcKrbR+CgdtotkZZYl3bRT7PQ5HG7BlL36EJOS4GsOZ9lhXqcKWQcTjRq8hNtL6a3t2LBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T06:09:02.118409Z"},"content_sha256":"f43af160a5f1d3df4f0b559f9e2cc142f0b4c23a65935cf4599895bec949c8fb","schema_version":"1.0","event_id":"sha256:f43af160a5f1d3df4f0b559f9e2cc142f0b4c23a65935cf4599895bec949c8fb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/bundle.json","state_url":"https://pith.science/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/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":"2026-06-02T06:09:02Z","links":{"resolver":"https://pith.science/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5","bundle":"https://pith.science/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/bundle.json","state":"https://pith.science/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/M2RM62M7G7UUL7V3ZWUPHVBGX5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:M2RM62M7G7UUL7V3ZWUPHVBGX5","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":"33d5dedfeeb570b7f871e9dfef91cf159a377ee91f1efc533887d2dc76b3d8d4","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-20T11:02:48Z","title_canon_sha256":"79886cbec5b10c43beb9ee0c8e9cd9f53593ef7e136aa52bbe32b5d2066bb1a7"},"schema_version":"1.0","source":{"id":"1804.07548","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1804.07548","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"arxiv_version","alias_value":"1804.07548v1","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.07548","created_at":"2026-05-18T00:13:26Z"},{"alias_kind":"pith_short_12","alias_value":"M2RM62M7G7UU","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"M2RM62M7G7UUL7V3","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"M2RM62M7","created_at":"2026-05-18T12:32:37Z"}],"graph_snapshots":[{"event_id":"sha256:f43af160a5f1d3df4f0b559f9e2cc142f0b4c23a65935cf4599895bec949c8fb","target":"graph","created_at":"2026-05-18T00:13:26Z","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 use a recent scaling analysis of the quasielastic electron scattering data from $^{12}$C to predict the quasielastic charge-changing neutrino scattering cross sections within an uncertainty band. We use a scaling function extracted from a selection of the $(e,e')$ cross section data, and an effective nucleon mass inspired by the relativistic mean-field model of nuclear matter. The corresponding super-scaling analysis with relativistic effective mass (SuSAM*) describes a large amount of the electron data lying inside a phenomenological quasielastic band. The effective mass incorporates the e","authors_text":"E. Ruiz Arriola, I. Ruiz Simo, J.E. Amaro, V.L. Martinez-Consentino","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-20T11:02:48Z","title":"Quasielastic charged-current neutrino scattering in the scaling model with relativistic effective mass"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.07548","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:e4f3de4db4399b32423da9243aeb15987bcf41fde029fd112c93d1a2e0d0309e","target":"record","created_at":"2026-05-18T00:13:26Z","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":"33d5dedfeeb570b7f871e9dfef91cf159a377ee91f1efc533887d2dc76b3d8d4","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-20T11:02:48Z","title_canon_sha256":"79886cbec5b10c43beb9ee0c8e9cd9f53593ef7e136aa52bbe32b5d2066bb1a7"},"schema_version":"1.0","source":{"id":"1804.07548","kind":"arxiv","version":1}},"canonical_sha256":"66a2cf699f37e945febbcda8f3d426bf5ed4b38789c09027d213da3fc77241ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"66a2cf699f37e945febbcda8f3d426bf5ed4b38789c09027d213da3fc77241ac","first_computed_at":"2026-05-18T00:13:26.105281Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:13:26.105281Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RhePmbQfh2fl7UTHsVusFj2oywcMWZeqg5hNHc21m4anVo5dLbiUIBr02GFWy3a+YUURkOqn1XB2Mr/fqs8ICg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:13:26.105959Z","signed_message":"canonical_sha256_bytes"},"source_id":"1804.07548","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e4f3de4db4399b32423da9243aeb15987bcf41fde029fd112c93d1a2e0d0309e","sha256:f43af160a5f1d3df4f0b559f9e2cc142f0b4c23a65935cf4599895bec949c8fb"],"state_sha256":"6ba536a5fa836c3a01422988b1563c8037ed1a26af0a8421d732fb77a0381988"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcBwTs5H05Fi56bxPnUj49NNUrDvA7i2GEmoDE0T0+UM1wLRwWT+vxm06KaEIi3VbL//KruNZ58+dlL33bD6Dw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T06:09:02.120651Z","bundle_sha256":"dfc4bb7c74d208d7acf058917c35f2c386197aa945a899028a9aac49348853cc"}}