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Prog. Phys."],"published-print":{"date-parts":[[2026,4,1]]},"abstract":"Abstract<\/jats:title>\n \n We review a theoretical framework for the cuprate superconductors, rooted in a fractionalized Fermi liquid (FL*) description of the intermediate-temperature pseudogap phase at low doping. The FL* theory predicted hole pockets each of fractional area\n \n \n \n <\/jats:tex-math>\n \n \n p<\/mml:mi>\n \n \/<\/mml:mo>\n <\/mml:mrow>\n 8<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:inline-formula>\n at hole doping\n p<\/jats:italic>\n , in contrast to the area\n \n \n \n <\/jats:tex-math>\n \n \n p<\/mml:mi>\n \n \/<\/mml:mo>\n <\/mml:mrow>\n 4<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:inline-formula>\n in spin density wave theory. Magnetotransport measurements, including observation of the Yamaji angle, show clear evidence of hole pocket quasiparticles which can tunnel coherently between square lattice layers, and are consistent with the FL* description. The FL* phase of a single-band model is described using a layer construction with a pair of ancilla qubits on each site: the Ancilla layer model (ALM). Its mean field theory yields hole pockets of area\n \n \n \n <\/jats:tex-math>\n \n \n p<\/mml:mi>\n \n \/<\/mml:mo>\n <\/mml:mrow>\n 8<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:inline-formula>\n , and matches the gapped photoemission spectrum in the anti-nodal region of the Brillouin zone. Fluctuations are described by the SU(2) gauge theory of a background spin liquid with critical Dirac spinons. A Monte Carlo study of the thermal SU(2) gauge theory transforms the hole pockets into Fermi arcs in photoemission. One route to confinement of FL* upon lowering temperature yields a\n d<\/jats:italic>\n -wave superconductor via a Kosterlitz\u2013Thouless transition of\n \n \n \n <\/jats:tex-math>\n \n \n h<\/mml:mi>\n \n \/<\/mml:mo>\n <\/mml:mrow>\n (<\/mml:mo>\n 2<\/mml:mn>\n e<\/mml:mi>\n )<\/mml:mo>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:inline-formula>\n vortices, with nodal Bogoliubov quasiparticles featuring anisotropic velocities and vortices surrounded by charge order halos. An alternative route yields a charge-ordered metallic state that has quantum oscillations consistent with observations. These confinement transitions are driven by the condensation of a SU(2) fundamental Higgs field, which also provides a fractionalized description of intertwined orders. Increasing doping from the FL* phase in the ALM drives a transition to a conventional FL at large doping, passing through an intermediate strange metal regime. We formulate a theory of the FL*-FL metal-metal transition without a symmetry-breaking order parameter, using a critical quantum \u2018charge\u2019 liquid of mobile electrons in the presence of disorder, developed via an extension of the Sachdev\u2013Ye\u2013Kitaev model to two spatial dimensions. At low temperatures, and across optimal and over doping, we address the regimes of extended non-FL behavior by Griffiths effects near quantum phase transitions in disordered metals.\n <\/jats:p>\n \n Partly based on lectures by S S at<\/jats:monospace>\n \n \n \n \n Boulder School 2025, Dynamics of Strongly Correlated Electrons<\/jats:ext-link>\n , 14\u201318 July.\n Lecture videos<\/jats:ext-link>\n .\n <\/jats:monospace>\n <\/jats:p>\n <\/jats:list-item>\n \n \n \n Joint ICTP-WE Heraeus School and Workshop on Advances in Quantum Matter: Pushing the Boundaries<\/jats:ext-link>\n , ICTP, Trieste, 4, 6 August 2025.\n Lecture videos<\/jats:ext-link>\n .\n <\/jats:monospace>\n <\/jats:p>\n <\/jats:list-item>\n \n \n \n School on Quantum Dynamics of Matter, Light and Information<\/jats:ext-link>\n , ICTP, Trieste, 18, 19 August 2025.\n Lecture videos<\/jats:ext-link>\n .\n <\/jats:monospace>\n <\/jats:p>\n <\/jats:list-item>\n \n \n \n Croucher Advanced Study Institute for Fractional Chern Insulators<\/jats:ext-link>\n , University of Hong Kong, 4, 5 September 2025.\n Lecture slides<\/jats:ext-link>\n .\n <\/jats:monospace>\n <\/jats:p>\n <\/jats:list-item>\n \n \n \n Advanced School and Conference on Quantum Matter<\/jats:ext-link>\n , ICTP Trieste, 1\u201312 December 2025.\n Lecture Notes<\/jats:ext-link>\n .\n Lecture videos<\/jats:ext-link>\n .\n <\/jats:monospace>\n <\/jats:p>\n <\/jats:list-item>\n <\/jats:list>\n <\/jats:p>","DOI":"10.1088\/1361-6633\/ae530d","type":"journal-article","created":{"date-parts":[[2026,3,17]],"date-time":"2026-03-17T22:49:28Z","timestamp":1773787768000},"page":"044501","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":10,"title":["Fractionalized Fermi liquids and the cuprate phase diagram"],"prefix":"10.1088","volume":"89","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-7465-7043","authenticated-orcid":true,"given":"Pietro M","family":"Bonetti","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0003-0116-5977","authenticated-orcid":false,"given":"Maine","family":"Christos","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-1232-5633","authenticated-orcid":false,"given":"Alexander","family":"Nikolaenko","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0001-7857-8724","authenticated-orcid":false,"given":"Aavishkar A","family":"Patel","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-2432-7070","authenticated-orcid":true,"given":"Subir","family":"Sachdev","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"266","published-online":{"date-parts":[[2026,4,16]]},"reference":[{"key":"ropae530dbib1","doi-asserted-by":"publisher","first-page":"537","DOI":"10.1002\/pssb.200983037","type":"journal-article","article-title":"Where is the quantum critical point in the cuprate superconductors?","volume":"247","author":"Sachdev","year":"2010","journal-title":"Phys. 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