{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:BYZML4CYH3U6C77EX2MRXWKI5B","short_pith_number":"pith:BYZML4CY","schema_version":"1.0","canonical_sha256":"0e32c5f0583ee9e17fe4be991bd948e86897e538d5b479ba633329383c6ea0e8","source":{"kind":"arxiv","id":"1209.3711","version":1},"attestation_state":"computed","paper":{"title":"Dynamical mass scale and approximate scaling symmetry in the Higgs sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Zygmunt Lalak","submitted_at":"2012-09-17T16:25:00Z","abstract_excerpt":"We investigate basic consequences of the assumption that the mass scale of the perturbative sector responsible for the spontaneous symmetry breaking is generated dynamically in a theory with a large UV scale. It is assumed that in addition to an elementary scalar there exists an additional scalar, a modulus, which controls the dynamical hierarchy of scales in the manner similar to that of supersymmetric gaugino condensation. It is shown that a light degree of freedom appears that couples to the gauge bosons and to charged fermions in a specific way which is different from the couplings of the "},"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":"1209.3711","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-09-17T16:25:00Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b6899108aa59741801b66741553f73fa33e9e95b2c35d06325c2956f9a5cbc2a","abstract_canon_sha256":"c65b0fe4add6cf10714f967ff8f60fe908a82b32be04803d8e663e365c1d1096"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:54:27.325879Z","signature_b64":"3uGedU8zL73X8u9N/Nj6NmFOu2eMzIFkdziGWvsbcOU0pn6Z/KblDE0nKRStQHhBONQjdfOl7U1is/KUm4foDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0e32c5f0583ee9e17fe4be991bd948e86897e538d5b479ba633329383c6ea0e8","last_reissued_at":"2026-05-18T01:54:27.325335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:54:27.325335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical mass scale and approximate scaling symmetry in the Higgs sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Zygmunt Lalak","submitted_at":"2012-09-17T16:25:00Z","abstract_excerpt":"We investigate basic consequences of the assumption that the mass scale of the perturbative sector responsible for the spontaneous symmetry breaking is generated dynamically in a theory with a large UV scale. It is assumed that in addition to an elementary scalar there exists an additional scalar, a modulus, which controls the dynamical hierarchy of scales in the manner similar to that of supersymmetric gaugino condensation. It is shown that a light degree of freedom appears that couples to the gauge bosons and to charged fermions in a specific way which is different from the couplings of the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.3711","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":"1209.3711","created_at":"2026-05-18T01:54:27.325431+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.3711v1","created_at":"2026-05-18T01:54:27.325431+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.3711","created_at":"2026-05-18T01:54:27.325431+00:00"},{"alias_kind":"pith_short_12","alias_value":"BYZML4CYH3U6","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_16","alias_value":"BYZML4CYH3U6C77E","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_8","alias_value":"BYZML4CY","created_at":"2026-05-18T12:27:01.376967+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/BYZML4CYH3U6C77EX2MRXWKI5B","json":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B.json","graph_json":"https://pith.science/api/pith-number/BYZML4CYH3U6C77EX2MRXWKI5B/graph.json","events_json":"https://pith.science/api/pith-number/BYZML4CYH3U6C77EX2MRXWKI5B/events.json","paper":"https://pith.science/paper/BYZML4CY"},"agent_actions":{"view_html":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B","download_json":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B.json","view_paper":"https://pith.science/paper/BYZML4CY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.3711&json=true","fetch_graph":"https://pith.science/api/pith-number/BYZML4CYH3U6C77EX2MRXWKI5B/graph.json","fetch_events":"https://pith.science/api/pith-number/BYZML4CYH3U6C77EX2MRXWKI5B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B/action/storage_attestation","attest_author":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B/action/author_attestation","sign_citation":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B/action/citation_signature","submit_replication":"https://pith.science/pith/BYZML4CYH3U6C77EX2MRXWKI5B/action/replication_record"}},"created_at":"2026-05-18T01:54:27.325431+00:00","updated_at":"2026-05-18T01:54:27.325431+00:00"}