{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:YX2UDTF5U72J36RU7PURFLEUUU","short_pith_number":"pith:YX2UDTF5","schema_version":"1.0","canonical_sha256":"c5f541ccbda7f49dfa34fbe912ac94a5368600140bc52595adae277f150eab32","source":{"kind":"arxiv","id":"1502.03028","version":2},"attestation_state":"computed","paper":{"title":"Two distinct kinetic regimes for the relaxation of light-induced superconductivity in La$_{1.675}$Eu$_{0.2}$Sr$_{0.125}$CuO$_{4}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"A. Cavalleri, C. R. Hunt, D. Nicoletti, H. Takagi, S. Kaiser, T. Takayama","submitted_at":"2015-02-10T18:30:02Z","abstract_excerpt":"We address the kinetic competition between charge striped order and superconductivity in La$_{1.675}$Eu$_{0.2}$Sr$_{0.125}$CuO$_{4}$. Ultrafast optical excitation is tuned to a mid-infrared vibrational resonance that destroys charge order and promptly establishes transient coherent interlayer coupling in this material. This effect is evidenced by the appearance of a longitudinal plasma mode reminiscent of a Josephson plasma resonance. We find that coherent interlayer coupling can be generated up to the charge order transition $T_{CO} \\approx$ 80 K, far above the equilibrium superconducting tra"},"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":"1502.03028","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2015-02-10T18:30:02Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"9b783b38628fab8794828f4462ac9fcc909278d6e7a1eac6a29d8973e7bc0f03","abstract_canon_sha256":"32381f70e4c6adff25690e535e4ce5f52e38a9400db6cb4818f2e23a4e1947d7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:25:55.497552Z","signature_b64":"r0HiioJcVwYBwAmub6NHyyXpdjcgcaeV4Aj6jknIEu1LEsB6hMWfQnzpfpdvJuSLNITOJznVeuocVnlY+rpbAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c5f541ccbda7f49dfa34fbe912ac94a5368600140bc52595adae277f150eab32","last_reissued_at":"2026-05-18T02:25:55.497153Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:25:55.497153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two distinct kinetic regimes for the relaxation of light-induced superconductivity in La$_{1.675}$Eu$_{0.2}$Sr$_{0.125}$CuO$_{4}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"A. Cavalleri, C. R. Hunt, D. Nicoletti, H. Takagi, S. Kaiser, T. Takayama","submitted_at":"2015-02-10T18:30:02Z","abstract_excerpt":"We address the kinetic competition between charge striped order and superconductivity in La$_{1.675}$Eu$_{0.2}$Sr$_{0.125}$CuO$_{4}$. Ultrafast optical excitation is tuned to a mid-infrared vibrational resonance that destroys charge order and promptly establishes transient coherent interlayer coupling in this material. This effect is evidenced by the appearance of a longitudinal plasma mode reminiscent of a Josephson plasma resonance. We find that coherent interlayer coupling can be generated up to the charge order transition $T_{CO} \\approx$ 80 K, far above the equilibrium superconducting tra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.03028","kind":"arxiv","version":2},"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":"1502.03028","created_at":"2026-05-18T02:25:55.497208+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.03028v2","created_at":"2026-05-18T02:25:55.497208+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.03028","created_at":"2026-05-18T02:25:55.497208+00:00"},{"alias_kind":"pith_short_12","alias_value":"YX2UDTF5U72J","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"YX2UDTF5U72J36RU","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"YX2UDTF5","created_at":"2026-05-18T12:29:52.810259+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/YX2UDTF5U72J36RU7PURFLEUUU","json":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU.json","graph_json":"https://pith.science/api/pith-number/YX2UDTF5U72J36RU7PURFLEUUU/graph.json","events_json":"https://pith.science/api/pith-number/YX2UDTF5U72J36RU7PURFLEUUU/events.json","paper":"https://pith.science/paper/YX2UDTF5"},"agent_actions":{"view_html":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU","download_json":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU.json","view_paper":"https://pith.science/paper/YX2UDTF5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.03028&json=true","fetch_graph":"https://pith.science/api/pith-number/YX2UDTF5U72J36RU7PURFLEUUU/graph.json","fetch_events":"https://pith.science/api/pith-number/YX2UDTF5U72J36RU7PURFLEUUU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU/action/storage_attestation","attest_author":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU/action/author_attestation","sign_citation":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU/action/citation_signature","submit_replication":"https://pith.science/pith/YX2UDTF5U72J36RU7PURFLEUUU/action/replication_record"}},"created_at":"2026-05-18T02:25:55.497208+00:00","updated_at":"2026-05-18T02:25:55.497208+00:00"}