{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:PLD6SON75T55NDO7O4Y5XRV7KD","short_pith_number":"pith:PLD6SON7","schema_version":"1.0","canonical_sha256":"7ac7e939bfecfbd68ddf7731dbc6bf50d367354c163e61a554b22d0779252c49","source":{"kind":"arxiv","id":"2405.09262","version":1},"attestation_state":"computed","paper":{"title":"Large solitons flattened by small quantum corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Eduard Kim, Emin Nugaev, Yakov Shnir","submitted_at":"2024-05-15T11:25:26Z","abstract_excerpt":"We propose a general form of the UV-completed Friedberg-Lee-Sirlin (FLS) model. As can be seen from the mechanical interpretation, UV-completion allows thin-wall approximation for non-topological solitons. The 1-loop renormalized effective potential for the UV-completed FLS model is constructed under the assumption of mass hierarchy. By special choice of parameters, we studied how the Coleman-Weinberg mechanism induces a new mass scale $\\omega_{-}$ in the classical FLS model. It can be expounded in terms of a stable condensate. As a consequence, the asymptotic of a non-topological soliton's en"},"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":"2405.09262","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-05-15T11:25:26Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"be49c5cd3e6a145a0d5bbb451508fcd0729e0c2eec15cacb75d4bb62e68ec48d","abstract_canon_sha256":"30ff987ceab3cac55083451011a64985726300e71829c187845f79fbeeec8b71"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:19:28.172625Z","signature_b64":"W1vws+MfxLvm9FC7JFeS8W2q4PoBvE5hX4wVKOJK70uLVzHuz96SnhxZpdxj8bDQ97MpSmiPtc/5uS7eRthpAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ac7e939bfecfbd68ddf7731dbc6bf50d367354c163e61a554b22d0779252c49","last_reissued_at":"2026-07-05T08:19:28.172247Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:19:28.172247Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large solitons flattened by small quantum corrections","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Eduard Kim, Emin Nugaev, Yakov Shnir","submitted_at":"2024-05-15T11:25:26Z","abstract_excerpt":"We propose a general form of the UV-completed Friedberg-Lee-Sirlin (FLS) model. As can be seen from the mechanical interpretation, UV-completion allows thin-wall approximation for non-topological solitons. The 1-loop renormalized effective potential for the UV-completed FLS model is constructed under the assumption of mass hierarchy. By special choice of parameters, we studied how the Coleman-Weinberg mechanism induces a new mass scale $\\omega_{-}$ in the classical FLS model. It can be expounded in terms of a stable condensate. As a consequence, the asymptotic of a non-topological soliton's en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.09262","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/2405.09262/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":"2405.09262","created_at":"2026-07-05T08:19:28.172302+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.09262v1","created_at":"2026-07-05T08:19:28.172302+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.09262","created_at":"2026-07-05T08:19:28.172302+00:00"},{"alias_kind":"pith_short_12","alias_value":"PLD6SON75T55","created_at":"2026-07-05T08:19:28.172302+00:00"},{"alias_kind":"pith_short_16","alias_value":"PLD6SON75T55NDO7","created_at":"2026-07-05T08:19:28.172302+00:00"},{"alias_kind":"pith_short_8","alias_value":"PLD6SON7","created_at":"2026-07-05T08:19:28.172302+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19917","citing_title":"Metastable and critical-bubble branches of Coleman--Weinberg monopoles","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2605.25243","citing_title":"Quantum-Corrected Q-balls in the Friedberg-Lee-Sirlin Model","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2604.04494","citing_title":"Multi-field oscillons/I-balls in the Friedberg-Lee-Sirlin model","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD","json":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD.json","graph_json":"https://pith.science/api/pith-number/PLD6SON75T55NDO7O4Y5XRV7KD/graph.json","events_json":"https://pith.science/api/pith-number/PLD6SON75T55NDO7O4Y5XRV7KD/events.json","paper":"https://pith.science/paper/PLD6SON7"},"agent_actions":{"view_html":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD","download_json":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD.json","view_paper":"https://pith.science/paper/PLD6SON7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.09262&json=true","fetch_graph":"https://pith.science/api/pith-number/PLD6SON75T55NDO7O4Y5XRV7KD/graph.json","fetch_events":"https://pith.science/api/pith-number/PLD6SON75T55NDO7O4Y5XRV7KD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD/action/storage_attestation","attest_author":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD/action/author_attestation","sign_citation":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD/action/citation_signature","submit_replication":"https://pith.science/pith/PLD6SON75T55NDO7O4Y5XRV7KD/action/replication_record"}},"created_at":"2026-07-05T08:19:28.172302+00:00","updated_at":"2026-07-05T08:19:28.172302+00:00"}