{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:MM675O75VIESQFTECBM3QXUSFS","short_pith_number":"pith:MM675O75","schema_version":"1.0","canonical_sha256":"633dfebbfdaa092816641059b85e922cbdbc5ad13f060ee5e7a196204205273f","source":{"kind":"arxiv","id":"1507.04233","version":1},"attestation_state":"computed","paper":{"title":"Modally Resolved Fabry-Perot Experiment with Semiconductor Waveguides","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"B. Pressl, C. Schneider, G. Weihs, J. Ge{\\ss}ler, K. Laiho, M. Kamp, S. H\\\"ofling, T. G\\\"unthner","submitted_at":"2015-07-15T14:32:22Z","abstract_excerpt":"Based on the interaction between different spatial modes, semiconductor Bragg-reflection waveguides provide a highly functional platform for non-linear optics. Therefore, the control and engineering of the properties of each spatial mode is essential. Despite the multimodeness of our waveguide, the well-established Fabry-Perot technique for recording fringes in the optical transmission spectrum can successfully be employed for a detailed linear optical characterization when combined with Fourier analysis. A prerequisite for the modal sensitivity is a finely resolved transmission spectrum that "},"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":"1507.04233","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-07-15T14:32:22Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"1a85be461a12d6051ca7334a7914229d1745515c4913b01821ece46619302a57","abstract_canon_sha256":"59f608923485579adfeba81e8599bf1b41c70f4244797b94f7caa853c35359ab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:15:58.452042Z","signature_b64":"KLPAWV+mdcEZgfQgGYrnfOsiqW7RmFPkhbcXF713z46OVdCc89oV2+AuFnqZKu3rVp72Jl45sXm2fMUseX0MDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"633dfebbfdaa092816641059b85e922cbdbc5ad13f060ee5e7a196204205273f","last_reissued_at":"2026-05-18T01:15:58.451362Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:15:58.451362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modally Resolved Fabry-Perot Experiment with Semiconductor Waveguides","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"B. Pressl, C. Schneider, G. Weihs, J. Ge{\\ss}ler, K. Laiho, M. Kamp, S. H\\\"ofling, T. G\\\"unthner","submitted_at":"2015-07-15T14:32:22Z","abstract_excerpt":"Based on the interaction between different spatial modes, semiconductor Bragg-reflection waveguides provide a highly functional platform for non-linear optics. Therefore, the control and engineering of the properties of each spatial mode is essential. Despite the multimodeness of our waveguide, the well-established Fabry-Perot technique for recording fringes in the optical transmission spectrum can successfully be employed for a detailed linear optical characterization when combined with Fourier analysis. A prerequisite for the modal sensitivity is a finely resolved transmission spectrum that "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.04233","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":"1507.04233","created_at":"2026-05-18T01:15:58.451458+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.04233v1","created_at":"2026-05-18T01:15:58.451458+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.04233","created_at":"2026-05-18T01:15:58.451458+00:00"},{"alias_kind":"pith_short_12","alias_value":"MM675O75VIES","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"MM675O75VIESQFTE","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"MM675O75","created_at":"2026-05-18T12:29:32.376354+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/MM675O75VIESQFTECBM3QXUSFS","json":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS.json","graph_json":"https://pith.science/api/pith-number/MM675O75VIESQFTECBM3QXUSFS/graph.json","events_json":"https://pith.science/api/pith-number/MM675O75VIESQFTECBM3QXUSFS/events.json","paper":"https://pith.science/paper/MM675O75"},"agent_actions":{"view_html":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS","download_json":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS.json","view_paper":"https://pith.science/paper/MM675O75","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.04233&json=true","fetch_graph":"https://pith.science/api/pith-number/MM675O75VIESQFTECBM3QXUSFS/graph.json","fetch_events":"https://pith.science/api/pith-number/MM675O75VIESQFTECBM3QXUSFS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS/action/storage_attestation","attest_author":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS/action/author_attestation","sign_citation":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS/action/citation_signature","submit_replication":"https://pith.science/pith/MM675O75VIESQFTECBM3QXUSFS/action/replication_record"}},"created_at":"2026-05-18T01:15:58.451458+00:00","updated_at":"2026-05-18T01:15:58.451458+00:00"}