{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:F3EM4QPVAJ43EAT3CCLGCIRZZ5","short_pith_number":"pith:F3EM4QPV","canonical_record":{"source":{"id":"1610.05624","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-18T14:12:05Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"c1c8d60a3f6c1372d363068b535f71212185ecd37dab787559988492a241dc42","abstract_canon_sha256":"e6a66b15ad8fd2eb32b1bb521b14a8b47a32c7a83b9a18fc3718b30bc92980ad"},"schema_version":"1.0"},"canonical_sha256":"2ec8ce41f50279b2027b1096612239cf4156fb80990d9a546ad19d0ffa66091a","source":{"kind":"arxiv","id":"1610.05624","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.05624","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"arxiv_version","alias_value":"1610.05624v2","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.05624","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"pith_short_12","alias_value":"F3EM4QPVAJ43","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"F3EM4QPVAJ43EAT3","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"F3EM4QPV","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:F3EM4QPVAJ43EAT3CCLGCIRZZ5","target":"record","payload":{"canonical_record":{"source":{"id":"1610.05624","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-18T14:12:05Z","cross_cats_sorted":["hep-ex","nucl-th"],"title_canon_sha256":"c1c8d60a3f6c1372d363068b535f71212185ecd37dab787559988492a241dc42","abstract_canon_sha256":"e6a66b15ad8fd2eb32b1bb521b14a8b47a32c7a83b9a18fc3718b30bc92980ad"},"schema_version":"1.0"},"canonical_sha256":"2ec8ce41f50279b2027b1096612239cf4156fb80990d9a546ad19d0ffa66091a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:52:09.109712Z","signature_b64":"6I4jjVEUekIDaLFshGALXYrb7AudO19HQs4doR2Z7jdvSbYx1QCKII7MJMqd+XY1YBs35s/c276Q7Eee1Xd2AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ec8ce41f50279b2027b1096612239cf4156fb80990d9a546ad19d0ffa66091a","last_reissued_at":"2026-05-18T00:52:09.109169Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:52:09.109169Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.05624","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":"2026-05-18T00:52:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ab4FDk7jARCvPOw9fPU4S1QXALEfu3NgPNKIe9bGQfWhgLk/7EhnjEEeAI305ELtznjzECeGJP+yU+QmckIXCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:56:02.485252Z"},"content_sha256":"d025433fc8f8d511cc4dbc09695639c13e8fc32dc981ee94da51639ec233253a","schema_version":"1.0","event_id":"sha256:d025433fc8f8d511cc4dbc09695639c13e8fc32dc981ee94da51639ec233253a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:F3EM4QPVAJ43EAT3CCLGCIRZZ5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Monte Carlo Implementation of Polarized Hadronization","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Anthony W. Thomas, Aram Kotzinian, Hrayr H. Matevosyan","submitted_at":"2016-10-18T14:12:05Z","abstract_excerpt":"We study the polarized quark hadronization in a Monte Carlo (MC) framework based on the recent extension of the quark-jet framework, where a self-consistent treatment of the quark polarization transfer in a sequential hadronization picture has been presented. Here, we first adopt this approach for MC simulations of hadronization process with finite number of produced hadrons, expressing the relevant probabilities in terms of the eight leading twist quark-to-quark transverse momentum dependent (TMD) splitting functions (SFs) for elementary $q \\to q'+h$ transition. We present explicit expression"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.05624","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":"2026-05-18T00:52:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6IBZpqMo1Q71yi/NZnVNACW+jwgVidEGt+V7m+79nbvMGJXAj2ETpwzn1qawJl2u5MJ2aVK/WfjdOv/agw5YCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:56:02.485930Z"},"content_sha256":"c6d473356e8bf25c1b5876dc4a4bbb75c16e100fba6a2074881b543822e8a0b6","schema_version":"1.0","event_id":"sha256:c6d473356e8bf25c1b5876dc4a4bbb75c16e100fba6a2074881b543822e8a0b6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/bundle.json","state_url":"https://pith.science/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/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":"2026-05-25T18:56:02Z","links":{"resolver":"https://pith.science/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5","bundle":"https://pith.science/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/bundle.json","state":"https://pith.science/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/F3EM4QPVAJ43EAT3CCLGCIRZZ5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:F3EM4QPVAJ43EAT3CCLGCIRZZ5","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":"e6a66b15ad8fd2eb32b1bb521b14a8b47a32c7a83b9a18fc3718b30bc92980ad","cross_cats_sorted":["hep-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-18T14:12:05Z","title_canon_sha256":"c1c8d60a3f6c1372d363068b535f71212185ecd37dab787559988492a241dc42"},"schema_version":"1.0","source":{"id":"1610.05624","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.05624","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"arxiv_version","alias_value":"1610.05624v2","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.05624","created_at":"2026-05-18T00:52:09Z"},{"alias_kind":"pith_short_12","alias_value":"F3EM4QPVAJ43","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"F3EM4QPVAJ43EAT3","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"F3EM4QPV","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:c6d473356e8bf25c1b5876dc4a4bbb75c16e100fba6a2074881b543822e8a0b6","target":"graph","created_at":"2026-05-18T00:52:09Z","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 study the polarized quark hadronization in a Monte Carlo (MC) framework based on the recent extension of the quark-jet framework, where a self-consistent treatment of the quark polarization transfer in a sequential hadronization picture has been presented. Here, we first adopt this approach for MC simulations of hadronization process with finite number of produced hadrons, expressing the relevant probabilities in terms of the eight leading twist quark-to-quark transverse momentum dependent (TMD) splitting functions (SFs) for elementary $q \\to q'+h$ transition. We present explicit expression","authors_text":"Anthony W. Thomas, Aram Kotzinian, Hrayr H. Matevosyan","cross_cats":["hep-ex","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-18T14:12:05Z","title":"Monte Carlo Implementation of Polarized Hadronization"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.05624","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:d025433fc8f8d511cc4dbc09695639c13e8fc32dc981ee94da51639ec233253a","target":"record","created_at":"2026-05-18T00:52:09Z","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":"e6a66b15ad8fd2eb32b1bb521b14a8b47a32c7a83b9a18fc3718b30bc92980ad","cross_cats_sorted":["hep-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-18T14:12:05Z","title_canon_sha256":"c1c8d60a3f6c1372d363068b535f71212185ecd37dab787559988492a241dc42"},"schema_version":"1.0","source":{"id":"1610.05624","kind":"arxiv","version":2}},"canonical_sha256":"2ec8ce41f50279b2027b1096612239cf4156fb80990d9a546ad19d0ffa66091a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2ec8ce41f50279b2027b1096612239cf4156fb80990d9a546ad19d0ffa66091a","first_computed_at":"2026-05-18T00:52:09.109169Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:52:09.109169Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6I4jjVEUekIDaLFshGALXYrb7AudO19HQs4doR2Z7jdvSbYx1QCKII7MJMqd+XY1YBs35s/c276Q7Eee1Xd2AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:52:09.109712Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.05624","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d025433fc8f8d511cc4dbc09695639c13e8fc32dc981ee94da51639ec233253a","sha256:c6d473356e8bf25c1b5876dc4a4bbb75c16e100fba6a2074881b543822e8a0b6"],"state_sha256":"b6d7fbac8bb308557427e9ec2f7b069d614dbd427ab7e8dd4c9baf6a40d6e708"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"95+GcSJRkw9LngpSJnpvC529QFke+6DRNF9oSuOfvhP0FHFt3iqlvhnMCe9jTT18R+8QAsFmf/YBe6XYglN9AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:56:02.490053Z","bundle_sha256":"1f2914ec0d2fba1194d862b73b8cf4b814f89fcca34054bcdd84c7b296a214bc"}}