{"record":{"author":{"account_ref":null,"orcid":null},"builds_on":[],"content_schema":"pubphys.content.revision/1","content_sha256":"64ad061d8cbd9a560af36361260f308ab2d1e7766baf8a0be3ac764dee0243d4","created":"2026-10-15T23:43:22Z","files":[],"origin":{"assisted_by":[],"kind":"seed"},"parents":["3ead336b9bdac11bd4f727aef256eb7a0334c3b6a1c52677bd4f3b0a080d1d01","ce59fb6cd812fc05906d0c60a71c75ea22bc686bcf38e7c3ef7010834d98ee7b"],"salt":"20ac1029a81d121c702c28c236a3ff1c5fbcc9bd812fa85b730e1f9cad40157a","schema":"pubphys.record/2","site":"pubphys.com","target":null,"type":"revision"},"content":{"answer_type":"yes-no","assisted_by":[],"external_id":"cm.iron-based.nematic-tc-enhancement","kind":"phenomenon","literature_status":"contested","n":"2","parents":[],"plain":"Near the point where nematic order disappears at zero temperature its fluctuations are strongest, and they might help electrons pair; data in different compounds disagree.","posed_since":"","precise":"In FeSe1-xSx the nematic transition vanishes near $x \\sim 0.17$ without a $T_{c}$ maximum, while in BaFe2(As1-xPx)2 and Ba(Fe1-xCox)2As2 nematic and magnetic critical points lie near the $T_{c}$ maximum. Determine whether nematic fluctuations contribute measurably to pairing given that coupling to lattice strain cuts off the divergence of the nematic correlation length. An answer is a quantitative estimate of the nematic contribution to the pairing interaction with an experimental test, such as $T_{c}$ versus nematic susceptibility under tuned strain.","problem_ref":"3ead336b9bdac11bd4f727aef256eb7a0334c3b6a1c52677bd4f3b0a080d1d01","references":"","settled_by":"Strain-tuned measurements of $T_{c}$ and nematic susceptibility in a single system with magnetic and nematic critical points separated, compared with a model calculation.","status_note":"","title":"Do nematic quantum critical fluctuations enhance $T_c$?","topic_ref":null},"attested":{"attestation":{"batch":null,"client_id":null,"id_token_sha256":null,"kind":"platform"},"record_hash":"b1160542e75336e6d2d588117aa82a74c34a0393b1018ac9bb40989905e2775b","schema":"pubphys.attested/1"},"envelope":{"attested_hash":"e42999e9f6cd01910233b105a16e151a67d4b53016996f8c02b91dd61d7d3334","platform_signature":{"key_id":"c6afc19b31429869751f06879c75cd64ea92654423d15b44be775bf1310a60da","sig":"Awe-j14tZvJNjkIokJOqkzl6mX6PPQe4OdQwmRYTDFMwrZLcrNImMF4CtnsjjgQbF7gsgFyIIor4N4OU6f7gDw"},"schema":"pubphys.envelope/1"},"record_hash":"b1160542e75336e6d2d588117aa82a74c34a0393b1018ac9bb40989905e2775b","leaf_index":2882}