It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
The properties of cuprate high-temperature superconductors are largely shaped by competing phases whose nature is often a mystery. Chiefly among them is the pseudogap phase, which sets in at a doping p* that is material-dependent. What determines p* is currently an open question. Here we show that the pseudogap cannot open on an electron-like Fermi surface, and can only exist below the doping pFS at which the large Fermi surface goes from hole-like to electron-like, so that p* ≤ pFS. We derive this result from high-magnetic-field transport measurements in La1.6−xNd0.4SrxCuO4 under pressure, which reveal a large and unexpected shift of p* with pressure, driven by a corresponding shift in pFS. This necessary condition for pseudogap formation, imposed by details of the Fermi surface, is a strong constraint for theories of the pseudogap phase. Our finding that p* can be tuned with a modest pressure opens a new route for experimental studies of the pseudogap.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details

1 Institut Quantique, Département de Physique & RQMP, Université de Sherbrooke, Sherbrooke, QC, Canada
2 Institut Quantique, Département de Physique & RQMP, Université de Sherbrooke, Sherbrooke, QC, Canada; Institute of Low Temperature and Structure Research, Polish Academy of Sciences, Wrocław, Poland
3 National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL, USA
4 École Polytechnique, CNRS, Université Paris-Saclay, Palaiseau, France; Collège de France, Paris, France
5 Materials Science and Engineering Program/Mechanical Engineering, University of Texas- Austin, Austin, TX, USA
6 Department of Applied Sciences, Muroran Institute of Technology, Muroran, Japan
7 Department of Physics, Hokkaido University, Sapporo, Japan
8 Department of Advanced Materials, University of Tokyo, Kashiwa, Japan
9 Institut Quantique, Département de Physique & RQMP, Université de Sherbrooke, Sherbrooke, QC, Canada; Canadian Institute for Advanced Research, Toronto, ON, Canada