{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:KUDRYRT32TO5KWDSJBFJ3LV345","short_pith_number":"pith:KUDRYRT3","canonical_record":{"source":{"id":"hep-ph/0108228","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-28T11:09:51Z","cross_cats_sorted":[],"title_canon_sha256":"175d47a8feee53347202aa4fa33ffb09434109dc13e1f017163b2f7c05563e6a","abstract_canon_sha256":"b0f40d1906f119910f23741f956d17015afac59ed5755b8b2213d8b800081562"},"schema_version":"1.0"},"canonical_sha256":"55071c467bd4ddd55872484a9daebbe765d834b7649a6ae8a5dde6fd49b1de28","source":{"kind":"arxiv","id":"hep-ph/0108228","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0108228","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0108228v1","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0108228","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"pith_short_12","alias_value":"KUDRYRT32TO5","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"KUDRYRT32TO5KWDS","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"KUDRYRT3","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:KUDRYRT32TO5KWDSJBFJ3LV345","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0108228","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-28T11:09:51Z","cross_cats_sorted":[],"title_canon_sha256":"175d47a8feee53347202aa4fa33ffb09434109dc13e1f017163b2f7c05563e6a","abstract_canon_sha256":"b0f40d1906f119910f23741f956d17015afac59ed5755b8b2213d8b800081562"},"schema_version":"1.0"},"canonical_sha256":"55071c467bd4ddd55872484a9daebbe765d834b7649a6ae8a5dde6fd49b1de28","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:36:39.420693Z","signature_b64":"bPcEfYleXPecnSSa5B6vlNlxxVfUYkJ3Y7eNAPfkJ0fYOwiymiWUPQ3l0pRloowzaKpuw2sqL6S0uunXdMBeDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"55071c467bd4ddd55872484a9daebbe765d834b7649a6ae8a5dde6fd49b1de28","last_reissued_at":"2026-05-18T02:36:39.420060Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:36:39.420060Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0108228","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":"2026-05-18T02:36:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AB0wFPe3H6hqOZxV5u8lMsUqfAihDsczINHV4TF3GZ6Vk8ugq3DfdzqryJ7n/93oN7WDDSTtMYgk0XcsIlugAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T19:35:55.909250Z"},"content_sha256":"d8f23cdb986c15faaf76b9a4d23d5bd1739b65c8bce70c7939728100d350771b","schema_version":"1.0","event_id":"sha256:d8f23cdb986c15faaf76b9a4d23d5bd1739b65c8bce70c7939728100d350771b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:KUDRYRT32TO5KWDSJBFJ3LV345","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Parton Distributions in Nucleon on the Basis of a Relativistic Independent Quark Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"N.Barik, R.N.Mishra","submitted_at":"2001-08-28T11:09:51Z","abstract_excerpt":"At a low resolution scale with $Q^2={\\mu}^2$ corresponding to the nucleon bound state; deep inelastic unpolarized structure functions $F_1(x,{\\mu}^2)$ and $F_2(x,{\\mu}^2)$ are derived with correct support using the symmetric part of the hadronic tensor under some simplifying assumptions in the Bjorken limit. For doing this; the nucleon in its ground state has been represented by a suitably constructed momentum wave packet of its valence quarks in their appropriate SU(6) spin flavor configuration with the momentum probability amplitude taken phenomenologically in reference to the independent qu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0108228","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":"2026-05-18T02:36:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1172LxhMnoOA7RuJvp4npQYZ3CQEAU/uuPcA9BK13EbW7zxdIfkD1ViGefT5oPGd/3mEZrHyJr55GF3e+JZuCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T19:35:55.909934Z"},"content_sha256":"a78726cfb68cd467a38c2c8d8148856a5bd439fd9769210ef3519881507688ad","schema_version":"1.0","event_id":"sha256:a78726cfb68cd467a38c2c8d8148856a5bd439fd9769210ef3519881507688ad"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KUDRYRT32TO5KWDSJBFJ3LV345/bundle.json","state_url":"https://pith.science/pith/KUDRYRT32TO5KWDSJBFJ3LV345/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KUDRYRT32TO5KWDSJBFJ3LV345/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":"2026-06-09T19:35:55Z","links":{"resolver":"https://pith.science/pith/KUDRYRT32TO5KWDSJBFJ3LV345","bundle":"https://pith.science/pith/KUDRYRT32TO5KWDSJBFJ3LV345/bundle.json","state":"https://pith.science/pith/KUDRYRT32TO5KWDSJBFJ3LV345/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KUDRYRT32TO5KWDSJBFJ3LV345/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:KUDRYRT32TO5KWDSJBFJ3LV345","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":"b0f40d1906f119910f23741f956d17015afac59ed5755b8b2213d8b800081562","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-28T11:09:51Z","title_canon_sha256":"175d47a8feee53347202aa4fa33ffb09434109dc13e1f017163b2f7c05563e6a"},"schema_version":"1.0","source":{"id":"hep-ph/0108228","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0108228","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0108228v1","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0108228","created_at":"2026-05-18T02:36:39Z"},{"alias_kind":"pith_short_12","alias_value":"KUDRYRT32TO5","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"KUDRYRT32TO5KWDS","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"KUDRYRT3","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:a78726cfb68cd467a38c2c8d8148856a5bd439fd9769210ef3519881507688ad","target":"graph","created_at":"2026-05-18T02:36:39Z","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":"At a low resolution scale with $Q^2={\\mu}^2$ corresponding to the nucleon bound state; deep inelastic unpolarized structure functions $F_1(x,{\\mu}^2)$ and $F_2(x,{\\mu}^2)$ are derived with correct support using the symmetric part of the hadronic tensor under some simplifying assumptions in the Bjorken limit. For doing this; the nucleon in its ground state has been represented by a suitably constructed momentum wave packet of its valence quarks in their appropriate SU(6) spin flavor configuration with the momentum probability amplitude taken phenomenologically in reference to the independent qu","authors_text":"N.Barik, R.N.Mishra","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2001-08-28T11:09:51Z","title":"Parton Distributions in Nucleon on the Basis of a Relativistic Independent Quark Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0108228","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:d8f23cdb986c15faaf76b9a4d23d5bd1739b65c8bce70c7939728100d350771b","target":"record","created_at":"2026-05-18T02:36:39Z","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":"b0f40d1906f119910f23741f956d17015afac59ed5755b8b2213d8b800081562","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2001-08-28T11:09:51Z","title_canon_sha256":"175d47a8feee53347202aa4fa33ffb09434109dc13e1f017163b2f7c05563e6a"},"schema_version":"1.0","source":{"id":"hep-ph/0108228","kind":"arxiv","version":1}},"canonical_sha256":"55071c467bd4ddd55872484a9daebbe765d834b7649a6ae8a5dde6fd49b1de28","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"55071c467bd4ddd55872484a9daebbe765d834b7649a6ae8a5dde6fd49b1de28","first_computed_at":"2026-05-18T02:36:39.420060Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:36:39.420060Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bPcEfYleXPecnSSa5B6vlNlxxVfUYkJ3Y7eNAPfkJ0fYOwiymiWUPQ3l0pRloowzaKpuw2sqL6S0uunXdMBeDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:36:39.420693Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0108228","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d8f23cdb986c15faaf76b9a4d23d5bd1739b65c8bce70c7939728100d350771b","sha256:a78726cfb68cd467a38c2c8d8148856a5bd439fd9769210ef3519881507688ad"],"state_sha256":"05daee2614f960192a80f07bbe4785402a4536ccf5ecab74eb1adf13c3837f44"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Zh/BeHwfcQxBKBU/lAVPtIeHdvLQ3XtL3dj2hKbbbGuEUa9O8K0+5CENpivaUymQXUPZMeM+dX6AF548sEcyBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T19:35:55.913888Z","bundle_sha256":"13fb06553a5a682a405496a7324b8c5c17bc7137c45a0a042d5a44734d5db98c"}}