{"id":2402,"date":"2026-07-16T04:00:00","date_gmt":"2026-07-16T04:00:00","guid":{"rendered":"https:\/\/futurenews24.com\/index.php\/2026\/07\/16\/2606-11056\/"},"modified":"2026-07-16T04:59:08","modified_gmt":"2026-07-16T04:59:08","slug":"2606-11056","status":"publish","type":"post","link":"https:\/\/futurenews24.com\/index.php\/2026\/07\/16\/2606-11056\/","title":{"rendered":"[2606.11056] On pseudogap section as precursor to a superconducting dome in high-Tc cuprates: Non-analytic T* as a perform of doping"},"content":{"rendered":"<p><br \/>\n<\/p>\n<div id=\"content-inner\">\n<div id=\"abs\">\n<div class=\"dateline\">\n  [Submitted on 9 Jun 2026 (v1), last revised 14 Jul 2026 (this version, v2)]<\/div>\n<p>View a PDF of the paper titled On pseudogap section as precursor to a superconducting dome in high-Tc cuprates: Non-analytic T* as a perform of doping, by Felix A. Buot<\/p>\n<p>    View PDF<br \/>\n    HTML (experimental)<\/p>\n<blockquote class=\"abstract mathjax\"><p>\n            <span class=\"descriptor\">Summary:<\/span>We generalize the situation beneath which a quantum materials exhibiting a pseudogap section is a precursor to a superconducting (SC) dome. The end result reveals the non-analytic T* as a perform of doping. A widely known instance is the high-Tc cuprates. Basically, the SC dome is generated beneath two circumstances: (1) that the pseudogap T* is a reducing perform of doping, because of the lower in measurement of prolonged pairing of doped holes with doping, and most significantly, (2) that the speed of configurational-ordering parameter is an rising perform of doping because of the lower in prolonged size of the disordered pairs. These two circumstances are offered by the brand new entanglement and confinement pairing mechanism of high-Tc cuprates. It is a concept that has lately been mentioned within the literature by Buot et al. It hinges on a novel robust entanglement and confinement gap pairing (ECHP) mechanism that unravels the microscopic options of all the section diagram of each electron and hole-doped high-Tc cuprates.\n    <\/p><\/blockquote><\/div>\n<\/div>\n<div>\n<h2>Submission historical past<\/h2>\n<p> From: Felix Buot Ph.D. [view email]                  [v1]<br \/>\n        Tue, 9 Jun 2026 16:20:06 UTC (217 KB)<br \/>\n    [v2]<br \/>\n        Tue, 14 Jul 2026 20:24:40 UTC (796 KB)\n<\/p><\/div>\n<p><br \/>\n<br \/><a href=\"https:\/\/arxiv.org\/abs\/2606.11056\">Source link <\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>[Submitted on 9 Jun 2026 (v1), last revised 14 Jul 2026 (this version, v2)] View a PDF of the paper titled On pseudogap section as precursor to a superconducting dome in high-Tc cuprates: Non-analytic T* as a perform of doping, by Felix A. Buot View PDF HTML (experimental) Summary:We generalize the situation beneath which a [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":2404,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"fifu_image_url":"http:\/\/arxiv.org\/static\/browse\/0.3.4\/images\/arxiv-logo-fb.png","fifu_image_alt":"","jnews-multi-image_gallery":[],"jnews_single_post":[],"jnews_primary_category":[],"jnews_override_bookmark_settings":[],"jnews_social_meta":[],"jnews_override_counter":[],"footnotes":""},"categories":[9],"tags":[2894,2892,2896,1740,2893,2895,1240,2891,2890,479],"class_list":["post-2402","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-quantum-computing","tag-cuprates","tag-dome","tag-doping","tag-function","tag-hightc","tag-nonanalytic","tag-phase","tag-precursor","tag-pseudogap","tag-superconducting"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.7 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>[2606.11056] On pseudogap section as precursor to a superconducting dome in high-Tc cuprates: Non-analytic T* as a perform of doping - 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