{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:RMJZ6KNDE5Y66CBB2T2R4KMDS3","short_pith_number":"pith:RMJZ6KND","schema_version":"1.0","canonical_sha256":"8b139f29a32771ef0821d4f51e298396fbd0c413bf9167509a5a8500e9cc4492","source":{"kind":"arxiv","id":"1711.08440","version":1},"attestation_state":"computed","paper":{"title":"Self-adjustment of a nonlinear lasing mode to a pumped area in a two-dimensional microcavity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD"],"primary_cat":"physics.optics","authors_text":"Satoshi Sunada, Susumu Shinohara, Takahisa Harayama, Yuta Kawashima","submitted_at":"2017-11-22T18:37:14Z","abstract_excerpt":"We numerically performed wave dynamical simulations based on the Maxwell-Bloch (MB) model for a quadrupole-deformed microcavity laser with spatially selective pumping. We demonstrate the appearance of an asymmetric lasing mode whose spatial pattern violates both the x- and y-axes mirror symmetries of the cavity. Dynamical simulations revealed that a lasing mode consisting of a clockwise or counterclockwise rotating-wave component is a stable stationary solution of the MB model. From the results of a passive-cavity mode analysis, we interpret these asymmetric rotating-wave lasing modes by the l"},"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":"1711.08440","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-11-22T18:37:14Z","cross_cats_sorted":["nlin.CD"],"title_canon_sha256":"8ad20c556094a097c086df73c0fc46263be29cb74d5db4875acc5798d68eacc8","abstract_canon_sha256":"6b5b5fb9d944e19b1116248e8b93a20d35ad906f4ae720db269901b4fd19fc02"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:49.795077Z","signature_b64":"1msg06gG4yAatlF+7axsOyVIZ28GepiGEkUcQT9OoVHKtxhwNhhHMX5oJf+zuhb9n1SV6vCOYlHIXEVfDyKLCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b139f29a32771ef0821d4f51e298396fbd0c413bf9167509a5a8500e9cc4492","last_reissued_at":"2026-05-18T00:29:49.794335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:49.794335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-adjustment of a nonlinear lasing mode to a pumped area in a two-dimensional microcavity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nlin.CD"],"primary_cat":"physics.optics","authors_text":"Satoshi Sunada, Susumu Shinohara, Takahisa Harayama, Yuta Kawashima","submitted_at":"2017-11-22T18:37:14Z","abstract_excerpt":"We numerically performed wave dynamical simulations based on the Maxwell-Bloch (MB) model for a quadrupole-deformed microcavity laser with spatially selective pumping. We demonstrate the appearance of an asymmetric lasing mode whose spatial pattern violates both the x- and y-axes mirror symmetries of the cavity. Dynamical simulations revealed that a lasing mode consisting of a clockwise or counterclockwise rotating-wave component is a stable stationary solution of the MB model. From the results of a passive-cavity mode analysis, we interpret these asymmetric rotating-wave lasing modes by the l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.08440","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":"1711.08440","created_at":"2026-05-18T00:29:49.794455+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.08440v1","created_at":"2026-05-18T00:29:49.794455+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.08440","created_at":"2026-05-18T00:29:49.794455+00:00"},{"alias_kind":"pith_short_12","alias_value":"RMJZ6KNDE5Y6","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_16","alias_value":"RMJZ6KNDE5Y66CBB","created_at":"2026-05-18T12:31:39.905425+00:00"},{"alias_kind":"pith_short_8","alias_value":"RMJZ6KND","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/RMJZ6KNDE5Y66CBB2T2R4KMDS3","json":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3.json","graph_json":"https://pith.science/api/pith-number/RMJZ6KNDE5Y66CBB2T2R4KMDS3/graph.json","events_json":"https://pith.science/api/pith-number/RMJZ6KNDE5Y66CBB2T2R4KMDS3/events.json","paper":"https://pith.science/paper/RMJZ6KND"},"agent_actions":{"view_html":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3","download_json":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3.json","view_paper":"https://pith.science/paper/RMJZ6KND","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.08440&json=true","fetch_graph":"https://pith.science/api/pith-number/RMJZ6KNDE5Y66CBB2T2R4KMDS3/graph.json","fetch_events":"https://pith.science/api/pith-number/RMJZ6KNDE5Y66CBB2T2R4KMDS3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3/action/storage_attestation","attest_author":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3/action/author_attestation","sign_citation":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3/action/citation_signature","submit_replication":"https://pith.science/pith/RMJZ6KNDE5Y66CBB2T2R4KMDS3/action/replication_record"}},"created_at":"2026-05-18T00:29:49.794455+00:00","updated_at":"2026-05-18T00:29:49.794455+00:00"}