{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:IVE5NQJVFD7BUEOSSE6DG3PJBN","short_pith_number":"pith:IVE5NQJV","schema_version":"1.0","canonical_sha256":"4549d6c13528fe1a11d2913c336de90b40ece19f210bb21e1a7170bf332b3cec","source":{"kind":"arxiv","id":"1304.4155","version":3},"attestation_state":"computed","paper":{"title":"Signatures of nonlinear cavity optomechanics in the weak coupling regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Nunnenkamp, J. D. Teufel, K. Borkje, S. M. Girvin","submitted_at":"2013-04-15T16:27:23Z","abstract_excerpt":"We identify signatures of the intrinsic nonlinear interaction between light and mechanical motion in cavity optomechanical systems. These signatures are observable even when the cavity linewidth exceeds the optomechanical coupling rate. A strong laser drive red-detuned by twice the mechanical frequency from the cavity resonance frequency makes two-phonon processes resonant, which leads to a nonlinear version of optomechanically induced transparency. This effect provides a new method of measuring the average phonon number of the mechanical oscillator. Furthermore, we show that if the strong las"},"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":"1304.4155","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2013-04-15T16:27:23Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"4d870f7d24e1b2abd06cf79ae95ef1cc632882a40cea312fe77782687b3e0052","abstract_canon_sha256":"9bc87daa19ad48c3094cfcb843c58b384ae29f7aafd6d6c93d44257242f867cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:18.837537Z","signature_b64":"fH0Do5odPsI/WKS85Xn/3ZJWvM1ay7eY9/mT4NSk+n9+DBOLJVG4A2+BlflsArS8q1f9gy832xZ+7+2xSgduCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4549d6c13528fe1a11d2913c336de90b40ece19f210bb21e1a7170bf332b3cec","last_reissued_at":"2026-05-18T03:16:18.836797Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:18.836797Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Signatures of nonlinear cavity optomechanics in the weak coupling regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"A. Nunnenkamp, J. D. Teufel, K. Borkje, S. M. Girvin","submitted_at":"2013-04-15T16:27:23Z","abstract_excerpt":"We identify signatures of the intrinsic nonlinear interaction between light and mechanical motion in cavity optomechanical systems. These signatures are observable even when the cavity linewidth exceeds the optomechanical coupling rate. A strong laser drive red-detuned by twice the mechanical frequency from the cavity resonance frequency makes two-phonon processes resonant, which leads to a nonlinear version of optomechanically induced transparency. This effect provides a new method of measuring the average phonon number of the mechanical oscillator. Furthermore, we show that if the strong las"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.4155","kind":"arxiv","version":3},"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":"1304.4155","created_at":"2026-05-18T03:16:18.836912+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.4155v3","created_at":"2026-05-18T03:16:18.836912+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.4155","created_at":"2026-05-18T03:16:18.836912+00:00"},{"alias_kind":"pith_short_12","alias_value":"IVE5NQJVFD7B","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_16","alias_value":"IVE5NQJVFD7BUEOS","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_8","alias_value":"IVE5NQJV","created_at":"2026-05-18T12:27:49.015174+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/IVE5NQJVFD7BUEOSSE6DG3PJBN","json":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN.json","graph_json":"https://pith.science/api/pith-number/IVE5NQJVFD7BUEOSSE6DG3PJBN/graph.json","events_json":"https://pith.science/api/pith-number/IVE5NQJVFD7BUEOSSE6DG3PJBN/events.json","paper":"https://pith.science/paper/IVE5NQJV"},"agent_actions":{"view_html":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN","download_json":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN.json","view_paper":"https://pith.science/paper/IVE5NQJV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.4155&json=true","fetch_graph":"https://pith.science/api/pith-number/IVE5NQJVFD7BUEOSSE6DG3PJBN/graph.json","fetch_events":"https://pith.science/api/pith-number/IVE5NQJVFD7BUEOSSE6DG3PJBN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN/action/storage_attestation","attest_author":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN/action/author_attestation","sign_citation":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN/action/citation_signature","submit_replication":"https://pith.science/pith/IVE5NQJVFD7BUEOSSE6DG3PJBN/action/replication_record"}},"created_at":"2026-05-18T03:16:18.836912+00:00","updated_at":"2026-05-18T03:16:18.836912+00:00"}