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Correction: van Delft et al. Two- and Three-Dimensional Superconducting Phases in the Weyl Semimetal TaP at Ambient Pressure. Crystals 2020, 10, 288

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König,  Markus
Markus König, Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Citation

van Delft, M., Pezzini, S., König, M., Tinnemans, P., Hussey, N., & Wiedmann, S. (2024). Correction: van Delft et al. Two- and Three-Dimensional Superconducting Phases in the Weyl Semimetal TaP at Ambient Pressure. Crystals 2020, 10, 288. Crystals, 14: 264, pp. 1-2. doi:10.3390/cryst14030264.


Cite as: https://hdl.handle.net/21.11116/0000-000F-378D-5
Abstract
In the original publication [1], there was a mistake in the equation for the 2D Tinkham model given in the Supplementary Materials, affecting main Figures 3a and S3b as published. This equation was erroneously stated as (Formula presented.) instead of the correct (Formula presented.) The corrected Figure 3 and Figure S3 appear below. (Figure presented.) (a) Angle dependence of the characteristic fields, fitted with the two-dimensional Tinkham model (solid lines) and the three-dimensional Ginzburg–Landau model (dashed lines). (b) Temperature dependence of the characteristic fields for parallel and perpendicular fields. H2 is fitted using a three-dimensional model and H1 with the two-dimensional Ginzburg–Landau model. H1 in a parallel field cannot be unambiguously identified and is thus omitted from this figure. Figure S3. Angle dependence of characteristic fields (extended version of main Figure 3), fitted with (a) the 3D Ginzburg–Landau model, (b) the 2D Tinkham model, (c) the Yamafuji model for thin films and (d) the Yamafuji model for surface superconductivity. The authors state that the scientific conclusions are unaffected. This correction was approved by the Academic Editor. The original publication has also been updated. © 2024 by the authors.