{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:WEPNJICUYL3XJECRG6ROQFYWMQ","short_pith_number":"pith:WEPNJICU","schema_version":"1.0","canonical_sha256":"b11ed4a054c2f774905137a2e817166428ed1b8daf40e07950361ecdabb84824","source":{"kind":"arxiv","id":"cond-mat/9609121","version":2},"attestation_state":"computed","paper":{"title":"Symmetry of the superconducting gap in $HgBa_{2}CaCu_{2}O_{6+\\delta}$ single crystals from electronic Raman scattering","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. Sacuto, D. Colson, N. Bontemps, P. Monod, R. Combescot, V. Viallet","submitted_at":"1996-09-13T11:46:20Z","abstract_excerpt":"Pure electronic Raman spectra with no phonon structures superimposed to the electronic continuum, are reported for the first time, in optimally doped $HgBa_{2}CaCu_{2}O_{6+\\delta } $ single crystals $(T_{c }=126 $ K). Our low temperature spectra (15 K) for the $A_{1g}$, $B_{1g} $ and $B_{2g} $ symmetries exhibit striking differences with previous data in $Bi_{2}Sr_{2}CaCu_{2}O_{8+\\delta }. $ The shape of the spectra for the various symmetries cannot be fitted by Devereaux's $d_{x^{2}-y^{2}} $ calculations, but strongly suggests a $d_{x y } $ gap, with its minima in the [100] and [010] directio"},"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/9609121","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-09-13T11:46:20Z","cross_cats_sorted":[],"title_canon_sha256":"68689ce11a849539dda68f7dfb0d234947dfb14775a78b9d4efcf2924b5039ae","abstract_canon_sha256":"c1ce959eda7fb95fc5d22def71cf7a27447929c9aa6439b9921252e3aa1ad431"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:34.004525Z","signature_b64":"btP/VwYva7Agilqf6kAkcYFCoePmeM2BMfxa7GhgzPYxsVNjMDgoMlPgmgEhldiPgwrKDNntfScpk+L2tbn2DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b11ed4a054c2f774905137a2e817166428ed1b8daf40e07950361ecdabb84824","last_reissued_at":"2026-05-18T01:39:34.003962Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:34.003962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Symmetry of the superconducting gap in $HgBa_{2}CaCu_{2}O_{6+\\delta}$ single crystals from electronic Raman scattering","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A. Sacuto, D. Colson, N. Bontemps, P. Monod, R. Combescot, V. Viallet","submitted_at":"1996-09-13T11:46:20Z","abstract_excerpt":"Pure electronic Raman spectra with no phonon structures superimposed to the electronic continuum, are reported for the first time, in optimally doped $HgBa_{2}CaCu_{2}O_{6+\\delta } $ single crystals $(T_{c }=126 $ K). Our low temperature spectra (15 K) for the $A_{1g}$, $B_{1g} $ and $B_{2g} $ symmetries exhibit striking differences with previous data in $Bi_{2}Sr_{2}CaCu_{2}O_{8+\\delta }. $ The shape of the spectra for the various symmetries cannot be fitted by Devereaux's $d_{x^{2}-y^{2}} $ calculations, but strongly suggests a $d_{x y } $ gap, with its minima in the [100] and [010] directio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9609121","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":"cond-mat/9609121","created_at":"2026-05-18T01:39:34.004049+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9609121v2","created_at":"2026-05-18T01:39:34.004049+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9609121","created_at":"2026-05-18T01:39:34.004049+00:00"},{"alias_kind":"pith_short_12","alias_value":"WEPNJICUYL3X","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"WEPNJICUYL3XJECR","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"WEPNJICU","created_at":"2026-05-18T12:25:48.327863+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/WEPNJICUYL3XJECRG6ROQFYWMQ","json":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ.json","graph_json":"https://pith.science/api/pith-number/WEPNJICUYL3XJECRG6ROQFYWMQ/graph.json","events_json":"https://pith.science/api/pith-number/WEPNJICUYL3XJECRG6ROQFYWMQ/events.json","paper":"https://pith.science/paper/WEPNJICU"},"agent_actions":{"view_html":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ","download_json":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ.json","view_paper":"https://pith.science/paper/WEPNJICU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9609121&json=true","fetch_graph":"https://pith.science/api/pith-number/WEPNJICUYL3XJECRG6ROQFYWMQ/graph.json","fetch_events":"https://pith.science/api/pith-number/WEPNJICUYL3XJECRG6ROQFYWMQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ/action/storage_attestation","attest_author":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ/action/author_attestation","sign_citation":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ/action/citation_signature","submit_replication":"https://pith.science/pith/WEPNJICUYL3XJECRG6ROQFYWMQ/action/replication_record"}},"created_at":"2026-05-18T01:39:34.004049+00:00","updated_at":"2026-05-18T01:39:34.004049+00:00"}