{"citation":{"ieee":"M. K. Chan <i>et al.</i>, “Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor,” <i>Nature Communications</i>, vol. 7. Springer Nature, 2016.","chicago":"Chan, M. K., N. Harrison, R. D. McDonald, B. J. Ramshaw, Kimberly A Modic, N. Barišić, and M. Greven. “Single Reconstructed Fermi Surface Pocket in an Underdoped Single-Layer Cuprate Superconductor.” <i>Nature Communications</i>. Springer Nature, 2016. <a href=\"https://doi.org/10.1038/ncomms12244\">https://doi.org/10.1038/ncomms12244</a>.","short":"M.K. Chan, N. Harrison, R.D. McDonald, B.J. Ramshaw, K.A. Modic, N. Barišić, M. Greven, Nature Communications 7 (2016).","mla":"Chan, M. K., et al. “Single Reconstructed Fermi Surface Pocket in an Underdoped Single-Layer Cuprate Superconductor.” <i>Nature Communications</i>, vol. 7, 12244, Springer Nature, 2016, doi:<a href=\"https://doi.org/10.1038/ncomms12244\">10.1038/ncomms12244</a>.","apa":"Chan, M. K., Harrison, N., McDonald, R. D., Ramshaw, B. J., Modic, K. A., Barišić, N., &#38; Greven, M. (2016). Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor. <i>Nature Communications</i>. Springer Nature. <a href=\"https://doi.org/10.1038/ncomms12244\">https://doi.org/10.1038/ncomms12244</a>","ista":"Chan MK, Harrison N, McDonald RD, Ramshaw BJ, Modic KA, Barišić N, Greven M. 2016. Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor. Nature Communications. 7, 12244.","ama":"Chan MK, Harrison N, McDonald RD, et al. Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor. <i>Nature Communications</i>. 2016;7. doi:<a href=\"https://doi.org/10.1038/ncomms12244\">10.1038/ncomms12244</a>"},"date_published":"2016-07-22T00:00:00Z","day":"22","year":"2016","user_id":"2DF688A6-F248-11E8-B48F-1D18A9856A87","_id":"7069","publication_status":"published","article_type":"original","language":[{"iso":"eng"}],"title":"Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor","intvolume":"         7","date_updated":"2021-01-12T08:11:41Z","month":"07","article_processing_charge":"No","quality_controlled":"1","author":[{"first_name":"M. K.","last_name":"Chan","full_name":"Chan, M. K."},{"full_name":"Harrison, N.","first_name":"N.","last_name":"Harrison"},{"first_name":"R. D.","last_name":"McDonald","full_name":"McDonald, R. D."},{"last_name":"Ramshaw","first_name":"B. J.","full_name":"Ramshaw, B. J."},{"orcid":"0000-0001-9760-3147","full_name":"Modic, Kimberly A","id":"13C26AC0-EB69-11E9-87C6-5F3BE6697425","last_name":"Modic","first_name":"Kimberly A"},{"last_name":"Barišić","first_name":"N.","full_name":"Barišić, N."},{"last_name":"Greven","first_name":"M.","full_name":"Greven, M."}],"publication_identifier":{"issn":["2041-1723"]},"article_number":"12244","doi":"10.1038/ncomms12244","volume":7,"oa_version":"Published Version","publication":"Nature Communications","date_created":"2019-11-19T13:21:23Z","publisher":"Springer Nature","extern":"1","type":"journal_article","status":"public","abstract":[{"text":"The observation of a reconstructed Fermi surface via quantum oscillations in hole-doped cuprates opened a path towards identifying broken symmetry states in the pseudogap regime. However, such an identification has remained inconclusive due to the multi-frequency quantum oscillation spectra and complications accounting for bilayer effects in most studies. We overcome these impediments with high-resolution measurements on the structurally simpler cuprate HgBa2CuO4+δ (Hg1201), which features one CuO2 plane per primitive unit cell. We find only a single oscillatory component with no signatures of magnetic breakdown tunnelling to additional orbits. Therefore, the Fermi surface comprises a single quasi-two-dimensional pocket. Quantitative modelling of these results indicates that a biaxial charge density wave within each CuO2 plane is responsible for the reconstruction and rules out criss-crossed charge stripes between layers as a viable alternative in Hg1201. Lastly, we determine that the characteristic gap between reconstructed pockets is a significant fraction of the pseudogap energy.","lang":"eng"}]}