{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:PN4HPMTVEUUPOGUJZNJAYLMPDR","short_pith_number":"pith:PN4HPMTV","schema_version":"1.0","canonical_sha256":"7b7877b2752528f71a89cb520c2d8f1c62df24bedd6fa0f7dad1dbd29264fe9c","source":{"kind":"arxiv","id":"2211.09021","version":2},"attestation_state":"computed","paper":{"title":"Ground state baryons in the flux-tube three-body confinement model using Diffusion Monte Carlo","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Lu Meng, Shi-Lin Zhu, Yan-Ke Chen, Yao Ma","submitted_at":"2022-11-16T16:28:13Z","abstract_excerpt":"We make a systematical diffusion Monte Carlo (DMC) calculation for all ground state baryons in two confinement scenarios, the pairwise confinement and the three-body flux-tube confinement. With the baryons as an example, we illustrate a feasible procedure to investigate the few-quark states with possible few-body confinement mechanisms, which can be extended to the multiquark states easily. For each baryon, we extract the mass, mean-square radius, charge radius, and the quark distributions. We use the Jackknife resampling method to estimate the statistical uncertainties of masses to be less th"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2211.09021","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-11-16T16:28:13Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"c8db50ee77980cec7b9b8f7cfa21d5f94be214501dfa184691272862dacd1385","abstract_canon_sha256":"25d0e3dca6d892b09b2f0b9a2a4fee9ff614bee86ac2195c6fa898f6fe8d512d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:55:14.589772Z","signature_b64":"/3i3ln3dgkVtR05DE6ZLF4ezUkpB7f8KEch2SlNgaNJ5iKq84UdZ/Z1RGc90ekCf8zV5Iz5zScXDv1k34bUfCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b7877b2752528f71a89cb520c2d8f1c62df24bedd6fa0f7dad1dbd29264fe9c","last_reissued_at":"2026-07-05T05:55:14.589279Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:55:14.589279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ground state baryons in the flux-tube three-body confinement model using Diffusion Monte Carlo","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"Lu Meng, Shi-Lin Zhu, Yan-Ke Chen, Yao Ma","submitted_at":"2022-11-16T16:28:13Z","abstract_excerpt":"We make a systematical diffusion Monte Carlo (DMC) calculation for all ground state baryons in two confinement scenarios, the pairwise confinement and the three-body flux-tube confinement. With the baryons as an example, we illustrate a feasible procedure to investigate the few-quark states with possible few-body confinement mechanisms, which can be extended to the multiquark states easily. For each baryon, we extract the mass, mean-square radius, charge radius, and the quark distributions. We use the Jackknife resampling method to estimate the statistical uncertainties of masses to be less th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.09021","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2211.09021/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2211.09021","created_at":"2026-07-05T05:55:14.589340+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.09021v2","created_at":"2026-07-05T05:55:14.589340+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.09021","created_at":"2026-07-05T05:55:14.589340+00:00"},{"alias_kind":"pith_short_12","alias_value":"PN4HPMTVEUUP","created_at":"2026-07-05T05:55:14.589340+00:00"},{"alias_kind":"pith_short_16","alias_value":"PN4HPMTVEUUPOGUJ","created_at":"2026-07-05T05:55:14.589340+00:00"},{"alias_kind":"pith_short_8","alias_value":"PN4HPMTV","created_at":"2026-07-05T05:55:14.589340+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.05502","citing_title":"Electromagnetic polarizabilities of the triplet hadrons in heavy hadron chiral perturbation theory","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR","json":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR.json","graph_json":"https://pith.science/api/pith-number/PN4HPMTVEUUPOGUJZNJAYLMPDR/graph.json","events_json":"https://pith.science/api/pith-number/PN4HPMTVEUUPOGUJZNJAYLMPDR/events.json","paper":"https://pith.science/paper/PN4HPMTV"},"agent_actions":{"view_html":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR","download_json":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR.json","view_paper":"https://pith.science/paper/PN4HPMTV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.09021&json=true","fetch_graph":"https://pith.science/api/pith-number/PN4HPMTVEUUPOGUJZNJAYLMPDR/graph.json","fetch_events":"https://pith.science/api/pith-number/PN4HPMTVEUUPOGUJZNJAYLMPDR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR/action/storage_attestation","attest_author":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR/action/author_attestation","sign_citation":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR/action/citation_signature","submit_replication":"https://pith.science/pith/PN4HPMTVEUUPOGUJZNJAYLMPDR/action/replication_record"}},"created_at":"2026-07-05T05:55:14.589340+00:00","updated_at":"2026-07-05T05:55:14.589340+00:00"}