<?xml version="1.0" encoding="UTF-8"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcq="http://purl.org/dc/terms/"><records count="1" morepages="false" start="1" end="1"><record rownumber="1"><dc:product_type>Journal Article</dc:product_type><dc:title>Deconfined quantum criticality of nodal &lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt; -wave superconductivity, Néel order, and charge order on the square lattice at half-filling</dc:title><dc:creator>Christos, Maine; Shackleton, Henry; Sachdev, Subir; Luo, Zhu-Xi</dc:creator><dc:corporate_author/><dc:editor/><dc:description>&lt;p&gt;We consider a SU(2) lattice gauge theory on the square lattice, with a single fundamental complex fermion and a single fundamental complex boson on each lattice site. Projective symmetries of the gauge-charged fermions are chosen so that they match with those of the spinons of the&lt;math&gt;&lt;mi&gt;π&lt;/mi&gt;&lt;/math&gt;-flux spin liquid. Global symmetries of all gauge-invariant observables are chosen to match with those of the particle-hole symmetric electronic Hubbard model at half-filling. Consequently, both the fundamental fermion and fundamental boson move in an average background&lt;math&gt;&lt;mi&gt;π&lt;/mi&gt;&lt;/math&gt;-flux, their gauge-invariant composite is the physical electron, and eliminating gauge fields in a strong gauge-coupling expansion yields an effective extended Hubbard model for the electrons. The SU(2) gauge theory displays several confining/Higgs phases: a nodal&lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt;-wave superconductor, and states with Néel, valence-bond solid, charge, or staggered current orders. There are also a number of quantum phase transitions between these phases that are very likely described by&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/math&gt;-dimensional deconfined conformal gauge theories, and we present large flavor expansions for such theories. These include the phenomenologically attractive case of a transition between a conventional insulator with a charge gap and Néel order, and a conventional&lt;math&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;/math&gt;-wave superconductor with gapless Bogoliubov quasiparticles at four nodal points in the Brillouin zone. We also apply our approach to the honeycomb lattice, where we find a bicritical point at the junction of Néel, valence bond solid (Kekulé), and Dirac semimetal phases.&lt;/p&gt; &lt;sec&gt;&lt;supplementary-material&gt;&lt;permissions&gt;&lt;copyright-statement&gt;Published by the American Physical Society&lt;/copyright-statement&gt;&lt;copyright-year&gt;2024&lt;/copyright-year&gt;&lt;/permissions&gt;&lt;/supplementary-material&gt;&lt;/sec&gt;</dc:description><dc:publisher>American Physical Society</dc:publisher><dc:date>2024-07-01</dc:date><dc:nsf_par_id>10521342</dc:nsf_par_id><dc:journal_name>Physical Review Research</dc:journal_name><dc:journal_volume>6</dc:journal_volume><dc:journal_issue>3</dc:journal_issue><dc:page_range_or_elocation/><dc:issn>2643-1564</dc:issn><dc:isbn/><dc:doi>https://doi.org/10.1103/PhysRevResearch.6.033018</dc:doi><dcq:identifierAwardId>2245246</dcq:identifierAwardId><dc:subject/><dc:version_number/><dc:location/><dc:rights/><dc:institution/><dc:sponsoring_org>National Science Foundation</dc:sponsoring_org></record></records></rdf:RDF>