{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:IZFPYCI2JWB2DEUKGDIQPVFEME","short_pith_number":"pith:IZFPYCI2","schema_version":"1.0","canonical_sha256":"464afc091a4d83a1928a30d107d4a4613efb7840cd62a50a4fa38d226bd61f6b","source":{"kind":"arxiv","id":"1301.2124","version":3},"attestation_state":"computed","paper":{"title":"A 125 GeV scalar improves the low-energy data support for the top-BESS model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Josef Juran, Mikulas Gintner","submitted_at":"2013-01-10T14:06:28Z","abstract_excerpt":"We investigate how adding a scalar resonance of a mass 125 GeV affects the low-energy data support for the top-BESS model as well as its low-energy free parameter limits. The top-BESS model is an effective Lagrangian, a modification of the well-known BESS model, with an ambition to describe phenomenology of the lowest bound states of strongly-interacting theories beyond the Standard model. In particular, the SU(2)_{L+R} vector resonance triplet of hypothetical bound states is a centerpiece of BESS-like effective models. The top-BESS model assumes that the triplet couples directly to the third "},"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":"1301.2124","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-01-10T14:06:28Z","cross_cats_sorted":[],"title_canon_sha256":"89d224dac7db6bd52a71b705df00c8472be73a29e78a054c7b4aef0beee56636","abstract_canon_sha256":"0a909a477cf6a3c53d6ea23d1046c0200497cdca2732bc68b1e92e34db80e1d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:12:11.891499Z","signature_b64":"vfKOoQd0ZWuaYoL89AKb5qoX9/mUj6R81CwM4+Zib5vM5Ng4fxnWPluQvSWB74OWRYGoK21X93s118mU0QYCDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"464afc091a4d83a1928a30d107d4a4613efb7840cd62a50a4fa38d226bd61f6b","last_reissued_at":"2026-05-18T03:12:11.890683Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:12:11.890683Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A 125 GeV scalar improves the low-energy data support for the top-BESS model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Josef Juran, Mikulas Gintner","submitted_at":"2013-01-10T14:06:28Z","abstract_excerpt":"We investigate how adding a scalar resonance of a mass 125 GeV affects the low-energy data support for the top-BESS model as well as its low-energy free parameter limits. The top-BESS model is an effective Lagrangian, a modification of the well-known BESS model, with an ambition to describe phenomenology of the lowest bound states of strongly-interacting theories beyond the Standard model. In particular, the SU(2)_{L+R} vector resonance triplet of hypothetical bound states is a centerpiece of BESS-like effective models. The top-BESS model assumes that the triplet couples directly to the third "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.2124","kind":"arxiv","version":3},"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":"1301.2124","created_at":"2026-05-18T03:12:11.890821+00:00"},{"alias_kind":"arxiv_version","alias_value":"1301.2124v3","created_at":"2026-05-18T03:12:11.890821+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.2124","created_at":"2026-05-18T03:12:11.890821+00:00"},{"alias_kind":"pith_short_12","alias_value":"IZFPYCI2JWB2","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_16","alias_value":"IZFPYCI2JWB2DEUK","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_8","alias_value":"IZFPYCI2","created_at":"2026-05-18T12:27:49.015174+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/IZFPYCI2JWB2DEUKGDIQPVFEME","json":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME.json","graph_json":"https://pith.science/api/pith-number/IZFPYCI2JWB2DEUKGDIQPVFEME/graph.json","events_json":"https://pith.science/api/pith-number/IZFPYCI2JWB2DEUKGDIQPVFEME/events.json","paper":"https://pith.science/paper/IZFPYCI2"},"agent_actions":{"view_html":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME","download_json":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME.json","view_paper":"https://pith.science/paper/IZFPYCI2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1301.2124&json=true","fetch_graph":"https://pith.science/api/pith-number/IZFPYCI2JWB2DEUKGDIQPVFEME/graph.json","fetch_events":"https://pith.science/api/pith-number/IZFPYCI2JWB2DEUKGDIQPVFEME/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME/action/storage_attestation","attest_author":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME/action/author_attestation","sign_citation":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME/action/citation_signature","submit_replication":"https://pith.science/pith/IZFPYCI2JWB2DEUKGDIQPVFEME/action/replication_record"}},"created_at":"2026-05-18T03:12:11.890821+00:00","updated_at":"2026-05-18T03:12:11.890821+00:00"}