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ZENODO
Dataset . 2023
License: CC BY
Data sources: Datacite
image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/
ZENODO
Dataset . 2023
License: CC BY
Data sources: Datacite
image/svg+xml art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos Open Access logo, converted into svg, designed by PLoS. This version with transparent background. http://commons.wikimedia.org/wiki/File:Open_Access_logo_PLoS_white.svg art designer at PLoS, modified by Wikipedia users Nina, Beao, JakobVoss, and AnonMoos http://www.plos.org/
ZENODO
Dataset . 2023
License: CC BY
Data sources: ZENODO
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Source Data for "Transport properties and doping evolution of the Fermi surface in cuprates"

Authors: Klebel-Knobloch, Benjamin; Tabiś, Wojciech; Gala, Mateusz A.; Barišić, Osor S.; Sunko, Denis K.; Barišić, Neven;

Source Data for "Transport properties and doping evolution of the Fermi surface in cuprates"

Abstract

Source data for the publication "Transport properties and doping evolution of the Fermi surface in cuprates", in Scientific Reports (https://doi.org/10.1038/s41598-023-39813-z) and on arxiv (https://doi.org/10.48550/arXiv.2303.05254). This dataset is organized in the following way: For every figure of the manuscript there is a separate folder, which includes the figure itself, as well as one or more additional folders for the individual panels. In those, there are one or more .csv files with the data. Some of the .csv files have two header lines, for example when the temperature and \(n_{\mathrm{H}}\) are recorded for multiple doping levels. Additional comments: Figure 1 The generic phase boundaries are not included. The precision of values of \(n_{\mathrm{loc}}\)is increased for presentation purposes experimental doping values are typically rounded to 2 decimal points, doping errors to 3 decimal points estimated \(n_{\mathrm{eff}}\) are rounded to 5 decimal points experimental \(n_{\mathrm{H}}\) from the literature are rounded to 3 decimal points otherwise, if it exists, experimental values are typically rounded to the error temperature is always given in Kelvin \(C_2\)is given in \([\mathrm{TK}^{-2}]\) (i.e. Tesla Kelvin^-2) the unit for \(n_{\mathrm{eff}}\), \(n_{\mathrm{loc}}\), \(n_{\mathrm{H}}\) is [per CuO2 unit cell] the unit for the resistivity in figure 4 is described in the methods section of the article

{"references": ["Bari\u0161i\u0107, N. et al., N. J. Phys. 21, 113007. https://doi.org/10.1088/1367-2630/ab4d0f (2019).", "Putzke, C. et al., Nat. Phys. 17, 826\u2013831. https://doi.org/10.1038/s41567-021-01197-0 (2021).", "Ayres, J. et al., Nature 595, 661\u2013666. https://doi.org/10.1038/s41586-021-03622-z (2021).", "Ando, Y. et al., Phys. Rev. Lett. 92, 197001. https://doi.org/10.1103/PhysRevLett.92.197001 (2004).", "Tsukada, I. et al., Phys. Rev. B 74, 134508. https://doi.org/10.1103/PhysRevB.74.134508 (2006).", "Padilla, W. J. et al., Phys. Rev. B 72, 060511. https://doi.org/10.1103/PhysRevB.72.060511 (2005).", "Bari\u0161i\u0107, N. et al., Proc. Natl. Acad. Sci. 110, 12235\u201312240. https://doi.org/10.1073/pnas.1301989110 (2013).", "Hussey, N. E. et al., J. Phys. Conf. Ser. 449, 012004. https://doi.org/10.1088/1742-6596/449/1/012004 (2013).", "Kaminski, A. et al., Phys. Rev. B 73, 174511. https://doi.org/10.1103/PhysRevB.73.174511 (2006).", "Culo, M. et al., SciPost Phys. 11, 012. https://doi.org/10.21468/SciPostPhys.11.1.012 (2021).", "Das, T., Phys. Rev. B 86, 054518. https://doi.org/10.1103/PhysRevB.86.054518 (2012).", "Vishik, I. M. et al., Phys. Rev. B 89, 195141. https://doi.org/10.1103/PhysRevB.89.195141 (2014).", "Plat\u00e9, M. et al., Phys. Rev. Lett. 95, 077001. https://doi.org/10.1103/PhysRevLett.95.077001 (2005)."]}

The work at the TU Wien was supported by the European Research Council (ERC Consolidator Grant No. 725521), while the work at the University of Zagreb was supported by project CeNIKS co-financed by the Croatian Government and the European Union through the European Regional Development Fund-Competitiveness and Cohesion Operational Programme (Grant No. KK.01.1.1.02.0013). The work at AGH University of Krakow was supported by the National Science Centre, Poland, Grant No. OPUS: UMO-2021/41/B/ST3/03454, the Polish National Agency for Academic Exchange under "Polish Returns 2019" Programme: PPN/PPO/2019/1/00014, and the subsidy of the Ministry of Science and Higher Education of Poland. M.A.G. was partly supported by program "Excellence Initiative – Research University" for AGH University of Krakow. O.S.B. acknowledges the support by the QuantiXLie Center of Excellence, a project co-financed by the Croatian Government and European Union through the European Regional Development Fund - the Competitiveness and Cohesion Operational Programme (Grant KK.01.1.1.01.0004).

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selected citations
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This is an alternative to the "Influence" indicator, which also reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Citations provided by BIP!
popularity
This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
BIP!Popularity provided by BIP!
influence
This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
BIP!Influence provided by BIP!
impulse
This indicator reflects the initial momentum of an article directly after its publication, based on the underlying citation network.
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