{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:B2VCHXFDOKVJG2HXGJ6K3EG64L","short_pith_number":"pith:B2VCHXFD","canonical_record":{"source":{"id":"1108.3204","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T11:15:00Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f5791bfc8ed23c125f9d6eb3110123136ebaa6e3e0af15ba2b822d5d356bcc94","abstract_canon_sha256":"a2ba5bff30cfa252dc0223779b73eb5f8a958a25f55654a859dceeebe5b3709d"},"schema_version":"1.0"},"canonical_sha256":"0eaa23dca372aa9368f7327cad90dee2e62bdf2df578e345ba6ea9265ddd5317","source":{"kind":"arxiv","id":"1108.3204","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.3204","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"arxiv_version","alias_value":"1108.3204v1","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.3204","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"pith_short_12","alias_value":"B2VCHXFDOKVJ","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"B2VCHXFDOKVJG2HX","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"B2VCHXFD","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:B2VCHXFDOKVJG2HXGJ6K3EG64L","target":"record","payload":{"canonical_record":{"source":{"id":"1108.3204","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T11:15:00Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f5791bfc8ed23c125f9d6eb3110123136ebaa6e3e0af15ba2b822d5d356bcc94","abstract_canon_sha256":"a2ba5bff30cfa252dc0223779b73eb5f8a958a25f55654a859dceeebe5b3709d"},"schema_version":"1.0"},"canonical_sha256":"0eaa23dca372aa9368f7327cad90dee2e62bdf2df578e345ba6ea9265ddd5317","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:53.354368Z","signature_b64":"mKpzlMV+orqTBFW6yXNcZdkL/YmHeTuNgKlJ6M5GaAYFyww870k1HuzVWjSTL18G5NsYQ4RW4UpsuGkcY8RdBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0eaa23dca372aa9368f7327cad90dee2e62bdf2df578e345ba6ea9265ddd5317","last_reissued_at":"2026-05-18T02:00:53.353798Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:53.353798Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1108.3204","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":"2026-05-18T02:00:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"msGTMwta6NhOpQUPD/vDbVuyNNqXT6jfe25Tnd+BOm7AdeyuR+QfP6/mBFugf762W1zKyHwCGGRlwOFh7T6zBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T20:33:54.741150Z"},"content_sha256":"9372c0a27b159ab890c24962ef64bde54b889fd04650ed085fd08242b722eca4","schema_version":"1.0","event_id":"sha256:9372c0a27b159ab890c24962ef64bde54b889fd04650ed085fd08242b722eca4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:B2VCHXFDOKVJG2HXGJ6K3EG64L","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transverse electron scattering response function of 3He in the quasi-elastic peak region and beyond with Delta isobar degrees of freedom","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Edward L. Tomusiak, Giuseppina Orlandini, Luping Yuan, Victor D. Efros, Winfried Leidemann","submitted_at":"2011-08-16T11:15:00Z","abstract_excerpt":"The 3He transverse electron scattering response function R_T(q,omega) is calculated in the quasi-elastic peak region and beyond for momentum transfers q = 500, 600 and 700 MeV/c. Distinct from our previous work for these kinematics where we included meson exchange currents and relativistic corrections we now additionally include Delta isobar currents (Delta-IC). The Delta-IC contribution increases the quasi-elastic peak height by about 5% and leads to an excellent agreement with experimental data in the whole peak region. In addition it is shown that effects due to the three-nucleon force larg"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.3204","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":"2026-05-18T02:00:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BgnP753cEAjKcbYpio2s0tyzpn5AtoDMkEQ1rD05B/DWU6vPmxWSqXF4VOEqlfHzFBhycIKNLqeQTjfY2P1iAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T20:33:54.741512Z"},"content_sha256":"2d32c0fcd828da8a95b5968773c81ef4fb15bc534ebb6f36494f341344392599","schema_version":"1.0","event_id":"sha256:2d32c0fcd828da8a95b5968773c81ef4fb15bc534ebb6f36494f341344392599"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/bundle.json","state_url":"https://pith.science/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/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":"2026-06-24T20:33:54Z","links":{"resolver":"https://pith.science/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L","bundle":"https://pith.science/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/bundle.json","state":"https://pith.science/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B2VCHXFDOKVJG2HXGJ6K3EG64L/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:B2VCHXFDOKVJG2HXGJ6K3EG64L","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":"a2ba5bff30cfa252dc0223779b73eb5f8a958a25f55654a859dceeebe5b3709d","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T11:15:00Z","title_canon_sha256":"f5791bfc8ed23c125f9d6eb3110123136ebaa6e3e0af15ba2b822d5d356bcc94"},"schema_version":"1.0","source":{"id":"1108.3204","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1108.3204","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"arxiv_version","alias_value":"1108.3204v1","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.3204","created_at":"2026-05-18T02:00:53Z"},{"alias_kind":"pith_short_12","alias_value":"B2VCHXFDOKVJ","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"B2VCHXFDOKVJG2HX","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"B2VCHXFD","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:2d32c0fcd828da8a95b5968773c81ef4fb15bc534ebb6f36494f341344392599","target":"graph","created_at":"2026-05-18T02:00:53Z","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 3He transverse electron scattering response function R_T(q,omega) is calculated in the quasi-elastic peak region and beyond for momentum transfers q = 500, 600 and 700 MeV/c. Distinct from our previous work for these kinematics where we included meson exchange currents and relativistic corrections we now additionally include Delta isobar currents (Delta-IC). The Delta-IC contribution increases the quasi-elastic peak height by about 5% and leads to an excellent agreement with experimental data in the whole peak region. In addition it is shown that effects due to the three-nucleon force larg","authors_text":"Edward L. Tomusiak, Giuseppina Orlandini, Luping Yuan, Victor D. Efros, Winfried Leidemann","cross_cats":["nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T11:15:00Z","title":"Transverse electron scattering response function of 3He in the quasi-elastic peak region and beyond with Delta isobar degrees of freedom"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.3204","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":"sha256:9372c0a27b159ab890c24962ef64bde54b889fd04650ed085fd08242b722eca4","target":"record","created_at":"2026-05-18T02:00:53Z","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":"a2ba5bff30cfa252dc0223779b73eb5f8a958a25f55654a859dceeebe5b3709d","cross_cats_sorted":["nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T11:15:00Z","title_canon_sha256":"f5791bfc8ed23c125f9d6eb3110123136ebaa6e3e0af15ba2b822d5d356bcc94"},"schema_version":"1.0","source":{"id":"1108.3204","kind":"arxiv","version":1}},"canonical_sha256":"0eaa23dca372aa9368f7327cad90dee2e62bdf2df578e345ba6ea9265ddd5317","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0eaa23dca372aa9368f7327cad90dee2e62bdf2df578e345ba6ea9265ddd5317","first_computed_at":"2026-05-18T02:00:53.353798Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:00:53.353798Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mKpzlMV+orqTBFW6yXNcZdkL/YmHeTuNgKlJ6M5GaAYFyww870k1HuzVWjSTL18G5NsYQ4RW4UpsuGkcY8RdBA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:00:53.354368Z","signed_message":"canonical_sha256_bytes"},"source_id":"1108.3204","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9372c0a27b159ab890c24962ef64bde54b889fd04650ed085fd08242b722eca4","sha256:2d32c0fcd828da8a95b5968773c81ef4fb15bc534ebb6f36494f341344392599"],"state_sha256":"ab5dd3e6ffe2990a5b2048004d5a6b7ad6ecda49758c984aa539a6a8af063cb1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E2ytKb3KfD99Pwx4hPtt/4aTPeTgKS0PPA5+tALeHuAXOZSR4paUnJvaW/FfrAGCuabFosiYZy20aK9wpNBtDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T20:33:54.743428Z","bundle_sha256":"9066917168b0fe40515e777adfabbe32048e36ed7df9e208ad7fbffd4ea3b3af"}}