{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RKLDXYUEM2NGR76JFUI47F6HUO","short_pith_number":"pith:RKLDXYUE","schema_version":"1.0","canonical_sha256":"8a963be284669a68ffc92d11cf97c7a397310f5f4da3563a23c304a489d56f5b","source":{"kind":"arxiv","id":"1706.01193","version":2},"attestation_state":"computed","paper":{"title":"Kink Dynamics in a Parametric $\\phi^6$ System: A Model With Controllably Many Internal Modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"nlin.PS","authors_text":"A. Demirkaya, A. Saxena, I. C. Christov, P. G. Kevrekidis, R. Decker","submitted_at":"2017-06-05T05:28:08Z","abstract_excerpt":"We explore a variant of the $\\phi^6$ model originally proposed in Phys.\\ Rev.\\ D {\\bf 12}, 1606 (1975) as a prototypical, so-called, \"bag\" model in which domain walls play the role of quarks within hadrons. We examine the steady state of the model, namely an apparent bound state of two kink structures. We explore its linearization, and we find that, as a function of a parameter controlling the curvature of the potential, an {\\it effectively arbitrary} number of internal modes may arise in the point spectrum of the linearization about the domain wall profile. We explore some of the key characte"},"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":"1706.01193","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2017-06-05T05:28:08Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"054a1f26ab1cad191c3926dabffdeccb996b30b454f540b0d47c2ee848bbf6f9","abstract_canon_sha256":"62a51a2df0c779e690d0682ec1b8e187d27b8fa1241b24edf07976274435e939"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:52.505592Z","signature_b64":"+hBW4ALA6c/4m0bOv/fE+0zxIC735VtrNVxZTFWVEY4qIMFqj9bJRasCSAjs2mVvGi4y2ifxUbS/QQwxz6HaCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a963be284669a68ffc92d11cf97c7a397310f5f4da3563a23c304a489d56f5b","last_reissued_at":"2026-05-18T00:27:52.504952Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:52.504952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kink Dynamics in a Parametric $\\phi^6$ System: A Model With Controllably Many Internal Modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"nlin.PS","authors_text":"A. Demirkaya, A. Saxena, I. C. Christov, P. G. Kevrekidis, R. Decker","submitted_at":"2017-06-05T05:28:08Z","abstract_excerpt":"We explore a variant of the $\\phi^6$ model originally proposed in Phys.\\ Rev.\\ D {\\bf 12}, 1606 (1975) as a prototypical, so-called, \"bag\" model in which domain walls play the role of quarks within hadrons. We examine the steady state of the model, namely an apparent bound state of two kink structures. We explore its linearization, and we find that, as a function of a parameter controlling the curvature of the potential, an {\\it effectively arbitrary} number of internal modes may arise in the point spectrum of the linearization about the domain wall profile. We explore some of the key characte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.01193","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":""},"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":"1706.01193","created_at":"2026-05-18T00:27:52.505076+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.01193v2","created_at":"2026-05-18T00:27:52.505076+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.01193","created_at":"2026-05-18T00:27:52.505076+00:00"},{"alias_kind":"pith_short_12","alias_value":"RKLDXYUEM2NG","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RKLDXYUEM2NGR76J","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RKLDXYUE","created_at":"2026-05-18T12:31:39.905425+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/RKLDXYUEM2NGR76JFUI47F6HUO","json":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO.json","graph_json":"https://pith.science/api/pith-number/RKLDXYUEM2NGR76JFUI47F6HUO/graph.json","events_json":"https://pith.science/api/pith-number/RKLDXYUEM2NGR76JFUI47F6HUO/events.json","paper":"https://pith.science/paper/RKLDXYUE"},"agent_actions":{"view_html":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO","download_json":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO.json","view_paper":"https://pith.science/paper/RKLDXYUE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.01193&json=true","fetch_graph":"https://pith.science/api/pith-number/RKLDXYUEM2NGR76JFUI47F6HUO/graph.json","fetch_events":"https://pith.science/api/pith-number/RKLDXYUEM2NGR76JFUI47F6HUO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO/action/storage_attestation","attest_author":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO/action/author_attestation","sign_citation":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO/action/citation_signature","submit_replication":"https://pith.science/pith/RKLDXYUEM2NGR76JFUI47F6HUO/action/replication_record"}},"created_at":"2026-05-18T00:27:52.505076+00:00","updated_at":"2026-05-18T00:27:52.505076+00:00"}