{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:U36DYS4TJUTB5RYJ4QRCTIDS6X","short_pith_number":"pith:U36DYS4T","schema_version":"1.0","canonical_sha256":"a6fc3c4b934d261ec709e42229a072f5e2641d3dbda6fcf316981ff553f5e23b","source":{"kind":"arxiv","id":"cond-mat/0207108","version":1},"attestation_state":"computed","paper":{"title":"Temperature dependence and mechanism of electrically detected ESR at the n=1 filling factor of a two-dimensional electron system in GaAs quantum wells","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Clifford R. Bowers, Eugene Olshanetsky, Jerry A. Simmons, John L. Reno, Joshua D. Caldwell, Manyam Pilla, Shu-chen Liu","submitted_at":"2002-07-03T17:10:59Z","abstract_excerpt":"Electrically detected electron spin resonance (EDESR) signals were acquired as a function of temperature in the 0.3-4.2 K temperature range in a AlGaAs/GaAs multiple quantum well sample at the filling factor at 5.7 T. In the particular sample studied, the line width is approximately temperature independent, while the amplitude exhibits a maximum at about 2.2 K and vanishes with increased or decreased temperature. To explain the observed temperature dependence of the signal amplitude, the signal amplitude temperature dependence is calculated assuming a model based on heating. The model ascribes"},"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":"cond-mat/0207108","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2002-07-03T17:10:59Z","cross_cats_sorted":[],"title_canon_sha256":"a30cdd0ef80dfdc54b5b9133f6ac32e2e4d8be8098965a5d23727f183df65d67","abstract_canon_sha256":"0d07f314b2c570e00d25e676c630ebe79b3198c25f8d338b6071e19976769322"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:32:34.960952Z","signature_b64":"C+EPgifuOMnG4oJwWvikfQeBkDnCyASws1+b/EVO4peIOdt76/lZX0WDzRj6FeKosjDjldRIP8sCR1i0jaxRDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a6fc3c4b934d261ec709e42229a072f5e2641d3dbda6fcf316981ff553f5e23b","last_reissued_at":"2026-07-04T16:32:34.960513Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:32:34.960513Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Temperature dependence and mechanism of electrically detected ESR at the n=1 filling factor of a two-dimensional electron system in GaAs quantum wells","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Clifford R. Bowers, Eugene Olshanetsky, Jerry A. Simmons, John L. Reno, Joshua D. Caldwell, Manyam Pilla, Shu-chen Liu","submitted_at":"2002-07-03T17:10:59Z","abstract_excerpt":"Electrically detected electron spin resonance (EDESR) signals were acquired as a function of temperature in the 0.3-4.2 K temperature range in a AlGaAs/GaAs multiple quantum well sample at the filling factor at 5.7 T. In the particular sample studied, the line width is approximately temperature independent, while the amplitude exhibits a maximum at about 2.2 K and vanishes with increased or decreased temperature. To explain the observed temperature dependence of the signal amplitude, the signal amplitude temperature dependence is calculated assuming a model based on heating. The model ascribes"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0207108","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/cond-mat/0207108/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":"cond-mat/0207108","created_at":"2026-07-04T16:32:34.960580+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0207108v1","created_at":"2026-07-04T16:32:34.960580+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0207108","created_at":"2026-07-04T16:32:34.960580+00:00"},{"alias_kind":"pith_short_12","alias_value":"U36DYS4TJUTB","created_at":"2026-07-04T16:32:34.960580+00:00"},{"alias_kind":"pith_short_16","alias_value":"U36DYS4TJUTB5RYJ","created_at":"2026-07-04T16:32:34.960580+00:00"},{"alias_kind":"pith_short_8","alias_value":"U36DYS4T","created_at":"2026-07-04T16:32:34.960580+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/U36DYS4TJUTB5RYJ4QRCTIDS6X","json":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X.json","graph_json":"https://pith.science/api/pith-number/U36DYS4TJUTB5RYJ4QRCTIDS6X/graph.json","events_json":"https://pith.science/api/pith-number/U36DYS4TJUTB5RYJ4QRCTIDS6X/events.json","paper":"https://pith.science/paper/U36DYS4T"},"agent_actions":{"view_html":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X","download_json":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X.json","view_paper":"https://pith.science/paper/U36DYS4T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0207108&json=true","fetch_graph":"https://pith.science/api/pith-number/U36DYS4TJUTB5RYJ4QRCTIDS6X/graph.json","fetch_events":"https://pith.science/api/pith-number/U36DYS4TJUTB5RYJ4QRCTIDS6X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X/action/storage_attestation","attest_author":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X/action/author_attestation","sign_citation":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X/action/citation_signature","submit_replication":"https://pith.science/pith/U36DYS4TJUTB5RYJ4QRCTIDS6X/action/replication_record"}},"created_at":"2026-07-04T16:32:34.960580+00:00","updated_at":"2026-07-04T16:32:34.960580+00:00"}