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. 2020 Sep 18;11:4707. doi: 10.1038/s41467-020-18540-3

Fig. 2. Low-energy electronic structure at the terminations of the Fe, Mn, and Co chains.

Fig. 2

a Constant-current scanning tunneling microscope (STM) image of the end of a Fe20 chain. b Differential tunneling conductance along the Fe20 chain aligned with the topography shown in (a). c dI/dV spectra of the Fe20 chain and substrate taken at the positions marked by crosses in (a) (Vstab = 1 mV, Istab = 0.2 nA, and Vmod = 20 µV). d dI/dV spectrum on the chain’s end from (c) normalized by subtraction of a spectrum averaged along the chain’s interior. e Constant-current STM image of the end of a Mn101 chain. f Differential tunneling conductance along the Mn101 chain. g dI/dV spectra of the Mn101 chain and substrate taken at the positions marked by crosses in (e) (Vstab = 1 mV, Istab = 0.5 nA, and Vmod = 40 µV). h dI/dV spectrum on the chain’s end from (g) normalized by subtraction of a spectrum averaged along the chain’s interior. i Constant-current STM image of the end of a Co84 chain. j Differential tunneling conductance along the Co84 chain. k dI/dV spectra of the Co84 chain and substrate taken at the positions marked by crosses in (i) (Vstab = 1 mV, Istab = 0.5 nA, and Vmod = 40 µV). l dI/dV spectrum on the chain’s end from (k) normalized by subtraction of a spectrum averaged along the chain’s interior. All data (a, e, i) are recorded with V = 6 mV, I = 0.2 nA. Arrows in (b, c, f, g): see text.