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<rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Unified description of cuprate superconductors using four-band $d$-$p$ model · HackerPapers discussions</title><link>https://hackerpaper.kaipfister.de/p/2105.11664/</link><description>Collected HN comments and submissions linking this paper.</description><language>en</language><lastBuildDate>Mon, 02 Nov 2026 11:16:22 GMT</lastBuildDate><atom:link href="https://hackerpaper.kaipfister.de/p/2105.11664/feed.xml" rel="self" type="application/rss+xml" /><item><title>Unified description of cuprate superconductors using four-band $d$-$p$ model — mentioned by bluecoconut</title><link>https://news.ycombinator.com/item?id=36966284</link><guid isPermaLink="false">urn:hackerpapers:mention:2105.11664:36966284</guid><pubDate>Wed, 02 Aug 2023 02:33:39 GMT</pubDate><description>&lt;p&gt;To be honest, this is a hunch thing more than a I can teach and explain it thing. To me it&amp;#x27;s just &amp;quot;a lot of the same stories&amp;quot; that are told about cuprates, and less of a &amp;quot;I can explain the mechanism&amp;quot;. Roughly, one of the &amp;quot;properties&amp;quot; that shows up with these materials is that the 3d orbitals of coper atoms are involved in forming the bands near the fermi level. Couple that with the fun story of Cu electron configuration being [Ar] 3d^10 4s^1, which suggests that spin-effects are &amp;quot;at play&amp;quot; with these electrons near their filling levels. Combine that with the spin-character properties of…&lt;/p&gt;&lt;p&gt;&lt;a href="https://hackerpaper.kaipfister.de/p/2105.11664/"&gt;Paper and discussion history&lt;/a&gt;. A mention is not an endorsement.&lt;/p&gt;</description><category>cond-mat.supr-con</category></item></channel></rss>
