{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:ZBO3FHOVLOB3VEBEOFRCNEM45A","short_pith_number":"pith:ZBO3FHOV","canonical_record":{"source":{"id":"hep-th/9401153","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-01-28T20:00:43Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"af08483f6f3d6698636d4b93ea3ac5ae3359d864a710914718301f44e197c130","abstract_canon_sha256":"64879fffd8dbdd2472543eec6d62f3a6efa99b6bf54d2b769a4536d97e195642"},"schema_version":"1.0"},"canonical_sha256":"c85db29dd55b83ba9024716226919ce80d0b7291c985ebccb71fc26c2f266c8d","source":{"kind":"arxiv","id":"hep-th/9401153","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9401153","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9401153v1","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9401153","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_12","alias_value":"ZBO3FHOVLOB3","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_16","alias_value":"ZBO3FHOVLOB3VEBE","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_8","alias_value":"ZBO3FHOV","created_at":"2026-07-04T15:57:40Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:ZBO3FHOVLOB3VEBEOFRCNEM45A","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9401153","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1994-01-28T20:00:43Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"af08483f6f3d6698636d4b93ea3ac5ae3359d864a710914718301f44e197c130","abstract_canon_sha256":"64879fffd8dbdd2472543eec6d62f3a6efa99b6bf54d2b769a4536d97e195642"},"schema_version":"1.0"},"canonical_sha256":"c85db29dd55b83ba9024716226919ce80d0b7291c985ebccb71fc26c2f266c8d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:57:40.682670Z","signature_b64":"0XHgIMTVYyVMhKjoP7vkIsZ5h8X7gLOa+Nx6+9yInSRIFV2qTi/S9TWTwxiZf4QebF4CXHWbGwnjHMAQFPWPDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c85db29dd55b83ba9024716226919ce80d0b7291c985ebccb71fc26c2f266c8d","last_reissued_at":"2026-07-04T15:57:40.682266Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:57:40.682266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9401153","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":"2026-07-04T15:57:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dTqVi+eyaMJICUJS77mt8H0+1rXFr3c2bR6Q6tZhbeHoY6Bo9ZEC4tG0vI/ye3WLdObsltwBGG4ll1azmGn+CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T15:26:28.537180Z"},"content_sha256":"dc8264486ed36c32189d1378be2d5da2fa55ac3393a75e254af3ae1ef0191186","schema_version":"1.0","event_id":"sha256:dc8264486ed36c32189d1378be2d5da2fa55ac3393a75e254af3ae1ef0191186"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:ZBO3FHOVLOB3VEBEOFRCNEM45A","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonperturbative Light-Front QCD","license":"","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-th","authors_text":"A. Harindranath, K. G. Wilson, R. J. Perry, S. Glazek, T. Walhout, W. M. Zhang","submitted_at":"1994-01-28T20:00:43Z","abstract_excerpt":"In this work the determination of low-energy bound states in Quantum Chromodynamics is recast so that it is linked to a weak-coupling problem. This allows one to approach the solution with the same techniques which solve Quantum Electrodynamics: namely, a combination of weak-coupling diagrams and many-body quantum mechanics. The key to eliminating necessarily nonperturbative effects is the use of a bare Hamiltonian in which quarks and gluons have nonzero constituent masses rather than the zero masses of the current picture. The use of constituent masses cuts off the growth of the running coupl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9401153","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9401153/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:57:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kVuy5HpRbQ3hnCDr22u7hHXcDE5j1Jj/pJIq+UZ6SgX3aQrQf6KJ44uVkwWNRDegdoaRKe9MsVVRezlTe1TFBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T15:26:28.537912Z"},"content_sha256":"ee9ad046f0deb2d821a46bc322d887f9b30436b4fa0e864768b56c11e2e98d5e","schema_version":"1.0","event_id":"sha256:ee9ad046f0deb2d821a46bc322d887f9b30436b4fa0e864768b56c11e2e98d5e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/bundle.json","state_url":"https://pith.science/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/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":"2026-08-11T15:26:28Z","links":{"resolver":"https://pith.science/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A","bundle":"https://pith.science/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/bundle.json","state":"https://pith.science/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZBO3FHOVLOB3VEBEOFRCNEM45A/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:ZBO3FHOVLOB3VEBEOFRCNEM45A","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":"64879fffd8dbdd2472543eec6d62f3a6efa99b6bf54d2b769a4536d97e195642","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1994-01-28T20:00:43Z","title_canon_sha256":"af08483f6f3d6698636d4b93ea3ac5ae3359d864a710914718301f44e197c130"},"schema_version":"1.0","source":{"id":"hep-th/9401153","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9401153","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9401153v1","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9401153","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_12","alias_value":"ZBO3FHOVLOB3","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_16","alias_value":"ZBO3FHOVLOB3VEBE","created_at":"2026-07-04T15:57:40Z"},{"alias_kind":"pith_short_8","alias_value":"ZBO3FHOV","created_at":"2026-07-04T15:57:40Z"}],"graph_snapshots":[{"event_id":"sha256:ee9ad046f0deb2d821a46bc322d887f9b30436b4fa0e864768b56c11e2e98d5e","target":"graph","created_at":"2026-07-04T15:57:40Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9401153/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work the determination of low-energy bound states in Quantum Chromodynamics is recast so that it is linked to a weak-coupling problem. This allows one to approach the solution with the same techniques which solve Quantum Electrodynamics: namely, a combination of weak-coupling diagrams and many-body quantum mechanics. The key to eliminating necessarily nonperturbative effects is the use of a bare Hamiltonian in which quarks and gluons have nonzero constituent masses rather than the zero masses of the current picture. The use of constituent masses cuts off the growth of the running coupl","authors_text":"A. Harindranath, K. G. Wilson, R. J. Perry, S. Glazek, T. Walhout, W. M. Zhang","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1994-01-28T20:00:43Z","title":"Nonperturbative Light-Front QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9401153","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:dc8264486ed36c32189d1378be2d5da2fa55ac3393a75e254af3ae1ef0191186","target":"record","created_at":"2026-07-04T15:57:40Z","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":"64879fffd8dbdd2472543eec6d62f3a6efa99b6bf54d2b769a4536d97e195642","cross_cats_sorted":["hep-ph","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1994-01-28T20:00:43Z","title_canon_sha256":"af08483f6f3d6698636d4b93ea3ac5ae3359d864a710914718301f44e197c130"},"schema_version":"1.0","source":{"id":"hep-th/9401153","kind":"arxiv","version":1}},"canonical_sha256":"c85db29dd55b83ba9024716226919ce80d0b7291c985ebccb71fc26c2f266c8d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c85db29dd55b83ba9024716226919ce80d0b7291c985ebccb71fc26c2f266c8d","first_computed_at":"2026-07-04T15:57:40.682266Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:57:40.682266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0XHgIMTVYyVMhKjoP7vkIsZ5h8X7gLOa+Nx6+9yInSRIFV2qTi/S9TWTwxiZf4QebF4CXHWbGwnjHMAQFPWPDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:57:40.682670Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9401153","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dc8264486ed36c32189d1378be2d5da2fa55ac3393a75e254af3ae1ef0191186","sha256:ee9ad046f0deb2d821a46bc322d887f9b30436b4fa0e864768b56c11e2e98d5e"],"state_sha256":"ee371ca586b78789ba89d6ef9eb386fe73f8f3a14ec371a367da356e0553f261"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v1ptTpKc9VB5GIQuJW8qXq01D/WOeVE4elUWQzmr3XJT1FCNBc/Ti/2aFD1BDNZzc8A/7JQm38j8+CDLdUYeCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T15:26:28.542695Z","bundle_sha256":"85e6417b4153e61463664b46b6790e7978806dd277aa3526feb760e5b0af6c38"}}