Fig. 2: Detecting surface magnetization from the tunnelling spectra. | Nature Physics

Fig. 2: Detecting surface magnetization from the tunnelling spectra.

From: Emergent exchange-driven giant magnetoelastic coupling in a correlated itinerant ferromagnet

Fig. 2: Detecting surface magnetization from the tunnelling spectra.

a, Sketch of the crystal structure of the top layers and magnetization of the bulk (MB) and surface layer (MS). In the ferromagnetic ground state26, both MS and MB point in the same direction parallel to the c axis (left). When the direction of one of them (here MB) is flipped (right), the exchange force results in an increase in the distance between the surface trilayer and the bulk (increase in the distance is exaggerated). b, Tunnelling spectra measured for parallel (black; MSMB) and antiparallel (purple; MSMB) alignment of the magnetizations of the bulk and surface layer. The spectra are normalized (norm.) by the value of g(V) at V = 8 mV. Two peaks are observed just below the Fermi level: PI and PII. The energy of peak PI (EPI) depends sensitively on the relative magnetization of the bulk and surface layer. It is 750 μV higher in energy when MB and MS are antiparallel compared with when they are parallel. The energy of peak PII (EPII) remains the same. c, Change in MS and MB observed in the tunnelling spectra taken between 0.41 T and –1.06 T, after having polarized the overall magnetization with Bz = 1.3 T. Triangles indicate PI, as in b. The energy of peak PI jumps abruptly to higher energies when MB switches between –0.13 T and –0.17 T, resulting in MS and MB being antiparallel. The peak jumps back when the surface layer switches between –0.96 T and –1.06 T. The spectra are offset vertically for clarity. d, Energy EPI of peak PI as a function of field Bz, taken by cycling the field from 1.3 T to –1.06 T and then back to 1.05 T. The direction of the triangles indicates the direction of the ramp of the field. PI changes abruptly at –0.16 T and –0.98 T when ramping to negative fields, and at 0.20 T and 0.96 T when ramping to a positive field. e, Energy EPI as a function of field Bz, taken by cycling Bz between –0.25 T and +0.25 T after aligning MB and MS with a field of Bz = –1 T. All data are taken at T = 80 mK (set-point conditions: Vset = 10 mV, Iset = 450 pA; lock-in modulation amplitude: VL = 125 μV). The points in d and e were extracted from a fit of two Lorentzian peaks to the spectra and the error bars are the 95% confidence intervals. The red and blue arrows illustrate the orientation of local moments at the surface (top line) and bulk (bottom line) along the cycle.

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