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. 2017 Apr 12;8:15036. doi: 10.1038/ncomms15036

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Copyright © 2017, The Author(s)

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(a) dc magnetization, M, and the real part of ac susceptibility, m′, as a function of in-plane magnetic field, H. For clarity, only data for Cs-intercalated BP are shown. Open symbols are data points measured as the dc field varied from −1 to +1 kOe and from +1 to −1 kOe. Solid lines show the same data smoothed using Savitzky–Golay filter. H_p and H_c denote the penetration and critical magnetic field, respectively. Inset: Zoomed-up m′ near the critical field in two orientations, with the arrows indicating and . (b,c) Temperature dependences of M(H) and m′(H). Only data for Cs_xBP are shown. Both types of measurements give the same values of T-dependent H_p and H_c.

Inline graphic — (a) dc magnetization, M, and the real part of ac susceptibility, m′, as a function of in-plane magnetic field, H. For clarity, only data for Cs-intercalated BP are shown. Open symbols are data points measured as the dc field varied from −1 to +1 kOe and from +1 to −1 kOe. Solid lines show the same data smoothed using Savitzky–Golay filter. H_p and H_c denote the penetration and critical magnetic field, respectively. Inset: Zoomed-up m′ near the critical field in two orientations, with the arrows indicating and . (b,c) Temperature dependences of M(H) and m′(H). Only data for Cs_xBP are shown. Both types of measurements give the same values of T-dependent H_p and H_c.