{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:RF27BEQ63FE5RPKDDCZB35LSIS","short_pith_number":"pith:RF27BEQ6","canonical_record":{"source":{"id":"1210.0634","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-02T02:15:39Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"6155233781164f1832dc4a5475a663238ea79fe223f079e6b66f56e2f22b87cd","abstract_canon_sha256":"ab45b3199add2b30f23f7cdb516747eca3f96d06e904704b06a6140a862c72b8"},"schema_version":"1.0"},"canonical_sha256":"8975f0921ed949d8bd4318b21df57244be3232ba7b35ef558dcacd6d0f3f2151","source":{"kind":"arxiv","id":"1210.0634","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.0634","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"arxiv_version","alias_value":"1210.0634v2","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0634","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"pith_short_12","alias_value":"RF27BEQ63FE5","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"RF27BEQ63FE5RPKD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"RF27BEQ6","created_at":"2026-05-18T12:27:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:RF27BEQ63FE5RPKDDCZB35LSIS","target":"record","payload":{"canonical_record":{"source":{"id":"1210.0634","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-02T02:15:39Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"6155233781164f1832dc4a5475a663238ea79fe223f079e6b66f56e2f22b87cd","abstract_canon_sha256":"ab45b3199add2b30f23f7cdb516747eca3f96d06e904704b06a6140a862c72b8"},"schema_version":"1.0"},"canonical_sha256":"8975f0921ed949d8bd4318b21df57244be3232ba7b35ef558dcacd6d0f3f2151","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:34:37.950746Z","signature_b64":"wNTB4ei28q+sQ0tRP7t6ki39HczqPc832VHal9KXAPvt5IMrOU30vSyr2hn9fGc1IEf7o3lDMmQyCjwjyxxQDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8975f0921ed949d8bd4318b21df57244be3232ba7b35ef558dcacd6d0f3f2151","last_reissued_at":"2026-05-18T03:34:37.949962Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:34:37.949962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.0634","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":"2026-05-18T03:34:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IqwECX3BkpjGKrBjYQ30OQMF2OWcK3GTG3bWos3dznbfxPvW3fbClwGECxyZJEH5VinNAhzuUg8C+DPbGXJzBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T23:48:56.568008Z"},"content_sha256":"bbacd146a59315f13ad9844c770f7e068adfbdae0b4bee00f1ac84e100e77f6d","schema_version":"1.0","event_id":"sha256:bbacd146a59315f13ad9844c770f7e068adfbdae0b4bee00f1ac84e100e77f6d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:RF27BEQ63FE5RPKDDCZB35LSIS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the physical meaning of Sachs form factors and on the violation of the dipole dependence of G_E and G_M on Q^2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"E. A. Kuraev, M. V. Galynskii","submitted_at":"2012-10-02T02:15:39Z","abstract_excerpt":"We discuss questions related to the interpretation of unexpected results of measurements of the proton form factors ratio G_E/G_M in the polarization experiments done in JLab in the region of 0.5 < Q^2 < 8.5 GeV^2. For this purpose, in the case of the hard scattering mechanism we calculated (in the leading approximation) the matrix elements of the proton current J^{\\pm \\delta,\\delta}_p for the full set of spin combinations corresponding to the number of the spin-flipped quarks, which contribute to the proton transition without spin-flip (J^{\\delta,\\delta}_p) and with the spin-flip (J^{-\\delta,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0634","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":"2026-05-18T03:34:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+guNcr72R6nE1IV68S2thC5V+I7wFvMWZA11VBX9pZ0gPhczikq30IxfYD2kAbdkzz9yqwoptoEVpoP8pP5tCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-18T23:48:56.568701Z"},"content_sha256":"00cc54efe82fce9ab0eb0e1176dc8033c2e613caf8eb45e169fa5894301d6990","schema_version":"1.0","event_id":"sha256:00cc54efe82fce9ab0eb0e1176dc8033c2e613caf8eb45e169fa5894301d6990"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RF27BEQ63FE5RPKDDCZB35LSIS/bundle.json","state_url":"https://pith.science/pith/RF27BEQ63FE5RPKDDCZB35LSIS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RF27BEQ63FE5RPKDDCZB35LSIS/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":"2026-05-18T23:48:56Z","links":{"resolver":"https://pith.science/pith/RF27BEQ63FE5RPKDDCZB35LSIS","bundle":"https://pith.science/pith/RF27BEQ63FE5RPKDDCZB35LSIS/bundle.json","state":"https://pith.science/pith/RF27BEQ63FE5RPKDDCZB35LSIS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RF27BEQ63FE5RPKDDCZB35LSIS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:RF27BEQ63FE5RPKDDCZB35LSIS","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":"ab45b3199add2b30f23f7cdb516747eca3f96d06e904704b06a6140a862c72b8","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-02T02:15:39Z","title_canon_sha256":"6155233781164f1832dc4a5475a663238ea79fe223f079e6b66f56e2f22b87cd"},"schema_version":"1.0","source":{"id":"1210.0634","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.0634","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"arxiv_version","alias_value":"1210.0634v2","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.0634","created_at":"2026-05-18T03:34:37Z"},{"alias_kind":"pith_short_12","alias_value":"RF27BEQ63FE5","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_16","alias_value":"RF27BEQ63FE5RPKD","created_at":"2026-05-18T12:27:20Z"},{"alias_kind":"pith_short_8","alias_value":"RF27BEQ6","created_at":"2026-05-18T12:27:20Z"}],"graph_snapshots":[{"event_id":"sha256:00cc54efe82fce9ab0eb0e1176dc8033c2e613caf8eb45e169fa5894301d6990","target":"graph","created_at":"2026-05-18T03:34:37Z","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 discuss questions related to the interpretation of unexpected results of measurements of the proton form factors ratio G_E/G_M in the polarization experiments done in JLab in the region of 0.5 < Q^2 < 8.5 GeV^2. For this purpose, in the case of the hard scattering mechanism we calculated (in the leading approximation) the matrix elements of the proton current J^{\\pm \\delta,\\delta}_p for the full set of spin combinations corresponding to the number of the spin-flipped quarks, which contribute to the proton transition without spin-flip (J^{\\delta,\\delta}_p) and with the spin-flip (J^{-\\delta,","authors_text":"E. A. Kuraev, M. V. Galynskii","cross_cats":["hep-ph","nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-02T02:15:39Z","title":"On the physical meaning of Sachs form factors and on the violation of the dipole dependence of G_E and G_M on Q^2"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.0634","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:bbacd146a59315f13ad9844c770f7e068adfbdae0b4bee00f1ac84e100e77f6d","target":"record","created_at":"2026-05-18T03:34:37Z","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":"ab45b3199add2b30f23f7cdb516747eca3f96d06e904704b06a6140a862c72b8","cross_cats_sorted":["hep-ph","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-10-02T02:15:39Z","title_canon_sha256":"6155233781164f1832dc4a5475a663238ea79fe223f079e6b66f56e2f22b87cd"},"schema_version":"1.0","source":{"id":"1210.0634","kind":"arxiv","version":2}},"canonical_sha256":"8975f0921ed949d8bd4318b21df57244be3232ba7b35ef558dcacd6d0f3f2151","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8975f0921ed949d8bd4318b21df57244be3232ba7b35ef558dcacd6d0f3f2151","first_computed_at":"2026-05-18T03:34:37.949962Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:34:37.949962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"wNTB4ei28q+sQ0tRP7t6ki39HczqPc832VHal9KXAPvt5IMrOU30vSyr2hn9fGc1IEf7o3lDMmQyCjwjyxxQDA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:34:37.950746Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.0634","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bbacd146a59315f13ad9844c770f7e068adfbdae0b4bee00f1ac84e100e77f6d","sha256:00cc54efe82fce9ab0eb0e1176dc8033c2e613caf8eb45e169fa5894301d6990"],"state_sha256":"becb3607e2db96e86a41ec566c3a68c4261ddec72ee79db73357af5a83522e84"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C6hZhlXwRLrPXtsbtVpBIBxSlykpPZnWBbvVHni2zA6PgXTU0yb4U0fZQ743BS+/k4exGpI+0uG9AkOVS+xsAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-18T23:48:56.570930Z","bundle_sha256":"49f8907bdff4f0f4f5d4feae5f2228053fbdb6abe912d64528c01137c3e6e6ca"}}