{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:B2QEZFYCZ6N4KIRBLXC7HOYFPU","short_pith_number":"pith:B2QEZFYC","canonical_record":{"source":{"id":"1009.5707","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-28T21:50:07Z","cross_cats_sorted":[],"title_canon_sha256":"9aedbfdbc409e84f11e494c3a31604c6b5fa30b7026f551085037d5eec745c24","abstract_canon_sha256":"55a5790abee5d549963e125c30dd01877337c36927b7c6659bac271a08fef4f5"},"schema_version":"1.0"},"canonical_sha256":"0ea04c9702cf9bc522215dc5f3bb057d1a8c213eac92c421ca7a025c1a046697","source":{"kind":"arxiv","id":"1009.5707","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.5707","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"arxiv_version","alias_value":"1009.5707v1","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.5707","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"pith_short_12","alias_value":"B2QEZFYCZ6N4","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"B2QEZFYCZ6N4KIRB","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"B2QEZFYC","created_at":"2026-05-18T12:26:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:B2QEZFYCZ6N4KIRBLXC7HOYFPU","target":"record","payload":{"canonical_record":{"source":{"id":"1009.5707","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-28T21:50:07Z","cross_cats_sorted":[],"title_canon_sha256":"9aedbfdbc409e84f11e494c3a31604c6b5fa30b7026f551085037d5eec745c24","abstract_canon_sha256":"55a5790abee5d549963e125c30dd01877337c36927b7c6659bac271a08fef4f5"},"schema_version":"1.0"},"canonical_sha256":"0ea04c9702cf9bc522215dc5f3bb057d1a8c213eac92c421ca7a025c1a046697","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:27:06.632614Z","signature_b64":"jGLBCbibTnePl1JCUl7jNs/0Cv+taC7Fdg2+B5QR7c9DYciIXuCK+FRyJtDuHabpqjrUdIQ0bOC+H/5loeVKDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ea04c9702cf9bc522215dc5f3bb057d1a8c213eac92c421ca7a025c1a046697","last_reissued_at":"2026-05-18T04:27:06.631915Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:27:06.631915Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1009.5707","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":"2026-05-18T04:27:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AfpdA3T333cqdCHzY6c5w/UESHLY1WLmPt/NeuERsmp5IUYDb9fnfBbjHlSqfP1Qn2VnB7wNyUYaWrYuQTUHDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:40:59.758358Z"},"content_sha256":"99f47759201599277034fd07a9ed7fce881dcb7861431da2bdfcfba2b293e92a","schema_version":"1.0","event_id":"sha256:99f47759201599277034fd07a9ed7fce881dcb7861431da2bdfcfba2b293e92a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:B2QEZFYCZ6N4KIRBLXC7HOYFPU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Generalized Transverse-Momentum Dependent Parton Distributions in Light-Cone Quark Models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Barbara Pasquini, C\\'edric Lorc\\'e","submitted_at":"2010-09-28T21:50:07Z","abstract_excerpt":"We discuss the general formalism for the calculation in light-cone quark models of the fully unintegrated, off-diagonal quark-quark correlator of the nucleon. The corresponding distributions in impact parameter space are the Wigner or phase-space distributions. The results obtained in two different light-cone quark models in the case of unpolarized quarks in an unpolarized proton are very similar and present a non-trivial shape which can be understood as due to the orbital motion of the quarks."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.5707","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":"2026-05-18T04:27:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"drPHUmr8hl6eepDRMjeNAmnpHNyIco2gWRFo2mvK0YYEMeCfzK4TT8aL2ezxEw/uhdSBa6fsz9zFP/hU71yvBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T23:40:59.759016Z"},"content_sha256":"021eec0dc09f14b986cfff8b3915de736de0194dffa2c661c64bce5ff2084628","schema_version":"1.0","event_id":"sha256:021eec0dc09f14b986cfff8b3915de736de0194dffa2c661c64bce5ff2084628"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/bundle.json","state_url":"https://pith.science/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/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":"2026-05-28T23:40:59Z","links":{"resolver":"https://pith.science/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU","bundle":"https://pith.science/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/bundle.json","state":"https://pith.science/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/B2QEZFYCZ6N4KIRBLXC7HOYFPU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:B2QEZFYCZ6N4KIRBLXC7HOYFPU","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":"55a5790abee5d549963e125c30dd01877337c36927b7c6659bac271a08fef4f5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-28T21:50:07Z","title_canon_sha256":"9aedbfdbc409e84f11e494c3a31604c6b5fa30b7026f551085037d5eec745c24"},"schema_version":"1.0","source":{"id":"1009.5707","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.5707","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"arxiv_version","alias_value":"1009.5707v1","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.5707","created_at":"2026-05-18T04:27:06Z"},{"alias_kind":"pith_short_12","alias_value":"B2QEZFYCZ6N4","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_16","alias_value":"B2QEZFYCZ6N4KIRB","created_at":"2026-05-18T12:26:05Z"},{"alias_kind":"pith_short_8","alias_value":"B2QEZFYC","created_at":"2026-05-18T12:26:05Z"}],"graph_snapshots":[{"event_id":"sha256:021eec0dc09f14b986cfff8b3915de736de0194dffa2c661c64bce5ff2084628","target":"graph","created_at":"2026-05-18T04:27:06Z","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 the general formalism for the calculation in light-cone quark models of the fully unintegrated, off-diagonal quark-quark correlator of the nucleon. The corresponding distributions in impact parameter space are the Wigner or phase-space distributions. The results obtained in two different light-cone quark models in the case of unpolarized quarks in an unpolarized proton are very similar and present a non-trivial shape which can be understood as due to the orbital motion of the quarks.","authors_text":"Barbara Pasquini, C\\'edric Lorc\\'e","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-28T21:50:07Z","title":"Generalized Transverse-Momentum Dependent Parton Distributions in Light-Cone Quark Models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.5707","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":"sha256:99f47759201599277034fd07a9ed7fce881dcb7861431da2bdfcfba2b293e92a","target":"record","created_at":"2026-05-18T04:27:06Z","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":"55a5790abee5d549963e125c30dd01877337c36927b7c6659bac271a08fef4f5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-28T21:50:07Z","title_canon_sha256":"9aedbfdbc409e84f11e494c3a31604c6b5fa30b7026f551085037d5eec745c24"},"schema_version":"1.0","source":{"id":"1009.5707","kind":"arxiv","version":1}},"canonical_sha256":"0ea04c9702cf9bc522215dc5f3bb057d1a8c213eac92c421ca7a025c1a046697","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0ea04c9702cf9bc522215dc5f3bb057d1a8c213eac92c421ca7a025c1a046697","first_computed_at":"2026-05-18T04:27:06.631915Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:27:06.631915Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jGLBCbibTnePl1JCUl7jNs/0Cv+taC7Fdg2+B5QR7c9DYciIXuCK+FRyJtDuHabpqjrUdIQ0bOC+H/5loeVKDw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:27:06.632614Z","signed_message":"canonical_sha256_bytes"},"source_id":"1009.5707","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:99f47759201599277034fd07a9ed7fce881dcb7861431da2bdfcfba2b293e92a","sha256:021eec0dc09f14b986cfff8b3915de736de0194dffa2c661c64bce5ff2084628"],"state_sha256":"817dd1567737240058dcd34a06e0d2724644c2fc38d67edb36f27a806c90d041"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZFhrmUQT3ARBHvuc4mx9ImLnchDc07bB3RwvZJYWm4Hc5T/Uatz7yzM3lRFsV21SMhRI9mf0GU/guV7i/LdvDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T23:40:59.762871Z","bundle_sha256":"dec022aed7b80c27877ac5195f52b8a8f411941d54b14d55661a618366616ae1"}}