{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:V5M7LYWI54KECT3V4HVVGHX52Q","short_pith_number":"pith:V5M7LYWI","schema_version":"1.0","canonical_sha256":"af59f5e2c8ef14414f75e1eb531efdd421b2d6acbdbd39faf7672e4beb78d0ea","source":{"kind":"arxiv","id":"1710.10216","version":1},"attestation_state":"computed","paper":{"title":"Testing a non-perturbative mechanism for elementary fermion mass generation: numerical results","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Bartosz Kostrzewa, Bastian Knippschild, Carsten Urbach, Ferenc Pittler, Giancarlo Rossi, Giulia Maria De Divitiis, Marco Garofalo, Petros Dimopoulos, Roberto Frezzotti, Stefano Capitani","submitted_at":"2017-10-27T16:02:25Z","abstract_excerpt":"Based on a recent proposal according to which elementary particle masses could be generated by a non-perturbative dynamical phenomenon, alternative to the Higgs mechanism, we carry out lattice simulations of a model where a non-abelian strongly interacting fermion doublet is also coupled to a doublet of complex scalar fields via a Yukawa and an \"irrelevant\" Wilson-like term. In this pioneering study we use naive fermions and work in the quenched approximation. We present preliminary numerical results both in the Wigner and in the Nambu-Goldstone phase, focusing on the observables relevant to c"},"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":"1710.10216","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-10-27T16:02:25Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"5ebbc78ee6b3bfa1875a2211374da53297f5c50c1c0ed68406a2e948938b2ea0","abstract_canon_sha256":"7f9e098b860b36b8a5190fce685ae182589241e58de234fa4346b56ded3d0f57"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:15.781606Z","signature_b64":"UHDxM0gDBvS2VJAOoxkfb9q22Yf04f99PZVEGKw5Cvsi4mxdFPcAu6HF0Hg2mcp7SEzr5vGDnjen9j3UV2GqDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af59f5e2c8ef14414f75e1eb531efdd421b2d6acbdbd39faf7672e4beb78d0ea","last_reissued_at":"2026-05-18T00:18:15.781078Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:15.781078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Testing a non-perturbative mechanism for elementary fermion mass generation: numerical results","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Bartosz Kostrzewa, Bastian Knippschild, Carsten Urbach, Ferenc Pittler, Giancarlo Rossi, Giulia Maria De Divitiis, Marco Garofalo, Petros Dimopoulos, Roberto Frezzotti, Stefano Capitani","submitted_at":"2017-10-27T16:02:25Z","abstract_excerpt":"Based on a recent proposal according to which elementary particle masses could be generated by a non-perturbative dynamical phenomenon, alternative to the Higgs mechanism, we carry out lattice simulations of a model where a non-abelian strongly interacting fermion doublet is also coupled to a doublet of complex scalar fields via a Yukawa and an \"irrelevant\" Wilson-like term. In this pioneering study we use naive fermions and work in the quenched approximation. We present preliminary numerical results both in the Wigner and in the Nambu-Goldstone phase, focusing on the observables relevant to c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.10216","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1710.10216","created_at":"2026-05-18T00:18:15.781166+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.10216v1","created_at":"2026-05-18T00:18:15.781166+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.10216","created_at":"2026-05-18T00:18:15.781166+00:00"},{"alias_kind":"pith_short_12","alias_value":"V5M7LYWI54KE","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"V5M7LYWI54KECT3V","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"V5M7LYWI","created_at":"2026-05-18T12:31:49.984773+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q","json":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q.json","graph_json":"https://pith.science/api/pith-number/V5M7LYWI54KECT3V4HVVGHX52Q/graph.json","events_json":"https://pith.science/api/pith-number/V5M7LYWI54KECT3V4HVVGHX52Q/events.json","paper":"https://pith.science/paper/V5M7LYWI"},"agent_actions":{"view_html":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q","download_json":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q.json","view_paper":"https://pith.science/paper/V5M7LYWI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.10216&json=true","fetch_graph":"https://pith.science/api/pith-number/V5M7LYWI54KECT3V4HVVGHX52Q/graph.json","fetch_events":"https://pith.science/api/pith-number/V5M7LYWI54KECT3V4HVVGHX52Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q/action/storage_attestation","attest_author":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q/action/author_attestation","sign_citation":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q/action/citation_signature","submit_replication":"https://pith.science/pith/V5M7LYWI54KECT3V4HVVGHX52Q/action/replication_record"}},"created_at":"2026-05-18T00:18:15.781166+00:00","updated_at":"2026-05-18T00:18:15.781166+00:00"}