{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:3OBOYXYUJ26GRKS2EAOTX7XTIJ","short_pith_number":"pith:3OBOYXYU","canonical_record":{"source":{"id":"nucl-th/0306002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2003-05-31T07:44:05Z","cross_cats_sorted":[],"title_canon_sha256":"519e139798abab736b9fbe0e5f45a988fe9e27a04fb0aae26b4b9c350fbbeb27","abstract_canon_sha256":"9b1c2b9d8f45bfe16a0bdfa801d04d4d02f18cd61069794849b7891fe17dfe6e"},"schema_version":"1.0"},"canonical_sha256":"db82ec5f144ebc68aa5a201d3bfef34255654a41761264a2a21fe794bb468f5d","source":{"kind":"arxiv","id":"nucl-th/0306002","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0306002","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0306002v1","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0306002","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"pith_short_12","alias_value":"3OBOYXYUJ26G","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"3OBOYXYUJ26GRKS2","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"3OBOYXYU","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:3OBOYXYUJ26GRKS2EAOTX7XTIJ","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0306002","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2003-05-31T07:44:05Z","cross_cats_sorted":[],"title_canon_sha256":"519e139798abab736b9fbe0e5f45a988fe9e27a04fb0aae26b4b9c350fbbeb27","abstract_canon_sha256":"9b1c2b9d8f45bfe16a0bdfa801d04d4d02f18cd61069794849b7891fe17dfe6e"},"schema_version":"1.0"},"canonical_sha256":"db82ec5f144ebc68aa5a201d3bfef34255654a41761264a2a21fe794bb468f5d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:14.247474Z","signature_b64":"xR8uMdu/PkpFTJanOnGp0MYMPTmzcENhrVkiXOiBBuacCJDSes3/0GG7ZuGVxXZ9gvtMHOz3s3Fd/HHP4a4LBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"db82ec5f144ebc68aa5a201d3bfef34255654a41761264a2a21fe794bb468f5d","last_reissued_at":"2026-05-18T01:38:14.246804Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:14.246804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0306002","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":"2026-05-18T01:38:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FKnXt+S9RjgEdHXnSRVsHz2uRzExTzmT2gVB/z3nSc1tcrBwPTJxABb6c3+0hBb0DR7eg5Ssxo7muB0pNj41BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:19:50.839807Z"},"content_sha256":"a1f06c7df123c480a51b0e4430a104e1394b2f7932b2bc433d07a3def53048b8","schema_version":"1.0","event_id":"sha256:a1f06c7df123c480a51b0e4430a104e1394b2f7932b2bc433d07a3def53048b8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:3OBOYXYUJ26GRKS2EAOTX7XTIJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scaling of Hadronic Form Factors in Point Form Kinematics","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. O. Riska, F.Coester","submitted_at":"2003-05-31T07:44:05Z","abstract_excerpt":"The general features of baryon form factors calculated with point form kinematics are derived. With point form kinematics and spectator currents hadronic form factors are functions of $\\eta:={1\\over 4}(v_{out}-v_{in})^2$ and, over a range of $\\eta$ values are insensitive to unitary scale transformations of the model wave functions when the extent of the wave function is small compared to the scale defined by the constituent mass, $<r^2 > \\ll 1/m^2$. The form factors are sensitive to the shape of such compact wave functions. Simple 3-quark proton wave functions are employed to illustrate these "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0306002","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":"2026-05-18T01:38:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ksbpDforN72XhIp9G8Mnx6vr7VHd+6oPjfZ51j/NYuKsaHF2SFCWDQs/fEiu7wnmmSvQuDSZFp9d005D1KcQAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:19:50.840435Z"},"content_sha256":"10716d835a0465022ff4b2081a566c08de3582a6aa8d8f3db751bd3c3977af06","schema_version":"1.0","event_id":"sha256:10716d835a0465022ff4b2081a566c08de3582a6aa8d8f3db751bd3c3977af06"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/bundle.json","state_url":"https://pith.science/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/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":"2026-05-27T02:19:50Z","links":{"resolver":"https://pith.science/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ","bundle":"https://pith.science/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/bundle.json","state":"https://pith.science/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3OBOYXYUJ26GRKS2EAOTX7XTIJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:3OBOYXYUJ26GRKS2EAOTX7XTIJ","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":"9b1c2b9d8f45bfe16a0bdfa801d04d4d02f18cd61069794849b7891fe17dfe6e","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2003-05-31T07:44:05Z","title_canon_sha256":"519e139798abab736b9fbe0e5f45a988fe9e27a04fb0aae26b4b9c350fbbeb27"},"schema_version":"1.0","source":{"id":"nucl-th/0306002","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0306002","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0306002v1","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0306002","created_at":"2026-05-18T01:38:14Z"},{"alias_kind":"pith_short_12","alias_value":"3OBOYXYUJ26G","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"3OBOYXYUJ26GRKS2","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"3OBOYXYU","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:10716d835a0465022ff4b2081a566c08de3582a6aa8d8f3db751bd3c3977af06","target":"graph","created_at":"2026-05-18T01:38:14Z","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 general features of baryon form factors calculated with point form kinematics are derived. With point form kinematics and spectator currents hadronic form factors are functions of $\\eta:={1\\over 4}(v_{out}-v_{in})^2$ and, over a range of $\\eta$ values are insensitive to unitary scale transformations of the model wave functions when the extent of the wave function is small compared to the scale defined by the constituent mass, $<r^2 > \\ll 1/m^2$. The form factors are sensitive to the shape of such compact wave functions. Simple 3-quark proton wave functions are employed to illustrate these ","authors_text":"D. O. Riska, F.Coester","cross_cats":[],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2003-05-31T07:44:05Z","title":"Scaling of Hadronic Form Factors in Point Form Kinematics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0306002","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:a1f06c7df123c480a51b0e4430a104e1394b2f7932b2bc433d07a3def53048b8","target":"record","created_at":"2026-05-18T01:38:14Z","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":"9b1c2b9d8f45bfe16a0bdfa801d04d4d02f18cd61069794849b7891fe17dfe6e","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2003-05-31T07:44:05Z","title_canon_sha256":"519e139798abab736b9fbe0e5f45a988fe9e27a04fb0aae26b4b9c350fbbeb27"},"schema_version":"1.0","source":{"id":"nucl-th/0306002","kind":"arxiv","version":1}},"canonical_sha256":"db82ec5f144ebc68aa5a201d3bfef34255654a41761264a2a21fe794bb468f5d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"db82ec5f144ebc68aa5a201d3bfef34255654a41761264a2a21fe794bb468f5d","first_computed_at":"2026-05-18T01:38:14.246804Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:14.246804Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xR8uMdu/PkpFTJanOnGp0MYMPTmzcENhrVkiXOiBBuacCJDSes3/0GG7ZuGVxXZ9gvtMHOz3s3Fd/HHP4a4LBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:14.247474Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0306002","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1f06c7df123c480a51b0e4430a104e1394b2f7932b2bc433d07a3def53048b8","sha256:10716d835a0465022ff4b2081a566c08de3582a6aa8d8f3db751bd3c3977af06"],"state_sha256":"3883f8931774aa8d1ee1bf1f3910fc7227a004edb113a880ba60d67e592329e8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fk+ur4ZNWneV/yjxAm1EqUxFiCa/TTiJUT+y22Wb4RHBZuPr1bQptVYTj8T4ETEQP9yqyVdtfp7V6XE8QyhrBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T02:19:50.843079Z","bundle_sha256":"304dc0139aa1dd782d7e7db9ef01ffe43e0a0b11cebdc01ee0a64aee60de20e1"}}