{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:T7LNUJY3662VHBCYTLXYSNGEHN","short_pith_number":"pith:T7LNUJY3","schema_version":"1.0","canonical_sha256":"9fd6da271bf7b55384589aef8934c43b7e6263c0c9d360a0cc880ff7a18781ac","source":{"kind":"arxiv","id":"1412.7295","version":1},"attestation_state":"computed","paper":{"title":"Theory of the electron phonon relaxation time in cuprates: Reproducing the observed temperature behaviour","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Navinder Singh, Pankaj Bhalla, Rukmani Bai","submitted_at":"2014-12-23T09:35:17Z","abstract_excerpt":"We have studied the temperature dependence of the rate of energy transfer from electronic sub-system to phononic sub-system in the case of cuprates, when the system is photo-excited by a femtosecond laser pulse. In the pseudogap state, taking the electronic dispersion {\\it as linear} near the nodal points of the Brillouin zone, we show that the rate of energy transfer from electronic sub-system to phononic sub-system is proportional to $T^{5}$ at lower temperatures ($T<<T_0$), and is proportional to $T$ at higher temperatures ($T>>T_0$), here $T_0$ is the Debye temperature for cuprates. The li"},"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":"1412.7295","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-12-23T09:35:17Z","cross_cats_sorted":[],"title_canon_sha256":"2fd024bf3cbbb1ac10a3184f942ad50fcb47ffa8ac3141d3df0f5e8e6a791298","abstract_canon_sha256":"c0e8b5bdb411ef3b67ad6b285694c86af11f81d22e6eab86cca5026c4216c976"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:30:39.198866Z","signature_b64":"b5A97E1N2lXd8kxx9TYDGTGZNBtOdo7ubnsZG+jhRIs5U0QuJJQEtI/Xqm2VdbQ2sYu1P/wr+GHx5gyUeKtbCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9fd6da271bf7b55384589aef8934c43b7e6263c0c9d360a0cc880ff7a18781ac","last_reissued_at":"2026-05-18T02:30:39.198388Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:30:39.198388Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of the electron phonon relaxation time in cuprates: Reproducing the observed temperature behaviour","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Navinder Singh, Pankaj Bhalla, Rukmani Bai","submitted_at":"2014-12-23T09:35:17Z","abstract_excerpt":"We have studied the temperature dependence of the rate of energy transfer from electronic sub-system to phononic sub-system in the case of cuprates, when the system is photo-excited by a femtosecond laser pulse. In the pseudogap state, taking the electronic dispersion {\\it as linear} near the nodal points of the Brillouin zone, we show that the rate of energy transfer from electronic sub-system to phononic sub-system is proportional to $T^{5}$ at lower temperatures ($T<<T_0$), and is proportional to $T$ at higher temperatures ($T>>T_0$), here $T_0$ is the Debye temperature for cuprates. The li"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.7295","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":"1412.7295","created_at":"2026-05-18T02:30:39.198451+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.7295v1","created_at":"2026-05-18T02:30:39.198451+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.7295","created_at":"2026-05-18T02:30:39.198451+00:00"},{"alias_kind":"pith_short_12","alias_value":"T7LNUJY3662V","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"T7LNUJY3662VHBCY","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"T7LNUJY3","created_at":"2026-05-18T12:28:49.207871+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/T7LNUJY3662VHBCYTLXYSNGEHN","json":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN.json","graph_json":"https://pith.science/api/pith-number/T7LNUJY3662VHBCYTLXYSNGEHN/graph.json","events_json":"https://pith.science/api/pith-number/T7LNUJY3662VHBCYTLXYSNGEHN/events.json","paper":"https://pith.science/paper/T7LNUJY3"},"agent_actions":{"view_html":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN","download_json":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN.json","view_paper":"https://pith.science/paper/T7LNUJY3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.7295&json=true","fetch_graph":"https://pith.science/api/pith-number/T7LNUJY3662VHBCYTLXYSNGEHN/graph.json","fetch_events":"https://pith.science/api/pith-number/T7LNUJY3662VHBCYTLXYSNGEHN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN/action/storage_attestation","attest_author":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN/action/author_attestation","sign_citation":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN/action/citation_signature","submit_replication":"https://pith.science/pith/T7LNUJY3662VHBCYTLXYSNGEHN/action/replication_record"}},"created_at":"2026-05-18T02:30:39.198451+00:00","updated_at":"2026-05-18T02:30:39.198451+00:00"}