{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:YNBFEUJCCVUMN23BPL2BOIAGFD","short_pith_number":"pith:YNBFEUJC","canonical_record":{"source":{"id":"hep-th/0310014","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-10-01T22:34:43Z","cross_cats_sorted":[],"title_canon_sha256":"4292d4944655adec64c777789c310a7a58a719aef126e9f5b0c6fc95bdc17e10","abstract_canon_sha256":"466dba8bac3c32e1f89aa2a5ff8ddc46afb44e6b5d79e00060169440a2808e33"},"schema_version":"1.0"},"canonical_sha256":"c3425251221568c6eb617af417200628c15700a832e0cb32e80db95a57f8a822","source":{"kind":"arxiv","id":"hep-th/0310014","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0310014","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0310014v1","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0310014","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"pith_short_12","alias_value":"YNBFEUJCCVUM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"YNBFEUJCCVUMN23B","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"YNBFEUJC","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:YNBFEUJCCVUMN23BPL2BOIAGFD","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0310014","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-10-01T22:34:43Z","cross_cats_sorted":[],"title_canon_sha256":"4292d4944655adec64c777789c310a7a58a719aef126e9f5b0c6fc95bdc17e10","abstract_canon_sha256":"466dba8bac3c32e1f89aa2a5ff8ddc46afb44e6b5d79e00060169440a2808e33"},"schema_version":"1.0"},"canonical_sha256":"c3425251221568c6eb617af417200628c15700a832e0cb32e80db95a57f8a822","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:40.183971Z","signature_b64":"9M3iH/K7BrwngN18CUoGIgi5zz8BNMqG+FZqRvHLQuF5p/lVAzFobYwLIT5n/uoQ5jSxa4BvhZnr+sAOzQm4Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3425251221568c6eb617af417200628c15700a832e0cb32e80db95a57f8a822","last_reissued_at":"2026-05-18T02:35:40.183391Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:40.183391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0310014","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":"2026-05-18T02:35:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"66IpIKXF6nFPp63Z7UmDLlBAABh+fCOoYmQ5IJAMpy0ji2XopYNFJ8rHFN6qt+nuKJcvlkdy8ZGNxWE6Eg7zDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T18:01:00.790777Z"},"content_sha256":"6d5bc4ec798f396f44df02c63163d1dcfb046a3d775e9e67aa87fb81a63da6b7","schema_version":"1.0","event_id":"sha256:6d5bc4ec798f396f44df02c63163d1dcfb046a3d775e9e67aa87fb81a63da6b7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:YNBFEUJCCVUMN23BPL2BOIAGFD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Parton Model from Bi-local Solitonic Picture of the Baryon in two-dimensions","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"G. S. Krishnaswami, S. G. Rajeev (University of Rochester), V. John","submitted_at":"2003-10-01T22:34:43Z","abstract_excerpt":"We study a previously introduced bi-local gauge invariant reformulation of two dimensional QCD, called 2d HadronDynamics. The baryon arises as a topological soliton in HadronDynamics. We derive an interacting parton model from the soliton model, thus reconciling these two seemingly different points of view. The valence quark model is obtained as a variational approximation to HadronDynamics. A succession of better approximations to the soliton picture are obtained. The next simplest case corresponds to a system of interacting valence, `sea' and anti-quarks. We also obtain this `embellished' pa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0310014","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":"2026-05-18T02:35:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lioftNYe6m7x0ZIjSCtj4606u1PC5Ts+WSDUitqS4Ppg2HvuYp+sXNfXp3+0uQ8X5opBIaagFFj+cf4Z7UBhAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-20T18:01:00.791430Z"},"content_sha256":"6e70734547d540bf1780d94888fb5a5e1d1d019df1808a9acdcb5f6cef2ec4da","schema_version":"1.0","event_id":"sha256:6e70734547d540bf1780d94888fb5a5e1d1d019df1808a9acdcb5f6cef2ec4da"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/bundle.json","state_url":"https://pith.science/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/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":"2026-05-20T18:01:00Z","links":{"resolver":"https://pith.science/pith/YNBFEUJCCVUMN23BPL2BOIAGFD","bundle":"https://pith.science/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/bundle.json","state":"https://pith.science/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YNBFEUJCCVUMN23BPL2BOIAGFD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:YNBFEUJCCVUMN23BPL2BOIAGFD","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":"466dba8bac3c32e1f89aa2a5ff8ddc46afb44e6b5d79e00060169440a2808e33","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-10-01T22:34:43Z","title_canon_sha256":"4292d4944655adec64c777789c310a7a58a719aef126e9f5b0c6fc95bdc17e10"},"schema_version":"1.0","source":{"id":"hep-th/0310014","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0310014","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0310014v1","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0310014","created_at":"2026-05-18T02:35:40Z"},{"alias_kind":"pith_short_12","alias_value":"YNBFEUJCCVUM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"YNBFEUJCCVUMN23B","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"YNBFEUJC","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:6e70734547d540bf1780d94888fb5a5e1d1d019df1808a9acdcb5f6cef2ec4da","target":"graph","created_at":"2026-05-18T02:35:40Z","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 a previously introduced bi-local gauge invariant reformulation of two dimensional QCD, called 2d HadronDynamics. The baryon arises as a topological soliton in HadronDynamics. We derive an interacting parton model from the soliton model, thus reconciling these two seemingly different points of view. The valence quark model is obtained as a variational approximation to HadronDynamics. A succession of better approximations to the soliton picture are obtained. The next simplest case corresponds to a system of interacting valence, `sea' and anti-quarks. We also obtain this `embellished' pa","authors_text":"G. S. Krishnaswami, S. G. Rajeev (University of Rochester), V. John","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-10-01T22:34:43Z","title":"Parton Model from Bi-local Solitonic Picture of the Baryon in two-dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0310014","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":"sha256:6d5bc4ec798f396f44df02c63163d1dcfb046a3d775e9e67aa87fb81a63da6b7","target":"record","created_at":"2026-05-18T02:35:40Z","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":"466dba8bac3c32e1f89aa2a5ff8ddc46afb44e6b5d79e00060169440a2808e33","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-10-01T22:34:43Z","title_canon_sha256":"4292d4944655adec64c777789c310a7a58a719aef126e9f5b0c6fc95bdc17e10"},"schema_version":"1.0","source":{"id":"hep-th/0310014","kind":"arxiv","version":1}},"canonical_sha256":"c3425251221568c6eb617af417200628c15700a832e0cb32e80db95a57f8a822","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c3425251221568c6eb617af417200628c15700a832e0cb32e80db95a57f8a822","first_computed_at":"2026-05-18T02:35:40.183391Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:35:40.183391Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9M3iH/K7BrwngN18CUoGIgi5zz8BNMqG+FZqRvHLQuF5p/lVAzFobYwLIT5n/uoQ5jSxa4BvhZnr+sAOzQm4Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:35:40.183971Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0310014","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6d5bc4ec798f396f44df02c63163d1dcfb046a3d775e9e67aa87fb81a63da6b7","sha256:6e70734547d540bf1780d94888fb5a5e1d1d019df1808a9acdcb5f6cef2ec4da"],"state_sha256":"a9efcff3b28b8d7d007e07d64584c67a08944837f1bdcceca4d5a6e56189c9a9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"M4EMJUGU4hFcEzvkVcsqxnxd2zxJ+J6NrRRytLZT3B6a7NGIyQkakpy0GVs2cSHO3vGCkSPWSlqFVkkb2ocoBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-20T18:01:00.793525Z","bundle_sha256":"e42973904af3347f755205dd8b161decacbf6ab95f7f5b5ea8f92fbe1d9ffe94"}}