Fig. 5: Scanning tunneling microscopy and spectroscopy investigation of rotation symmetry breaking in ScV6Sn6, and the comparison to KV3Sb5. | npj Quantum Materials

Fig. 5: Scanning tunneling microscopy and spectroscopy investigation of rotation symmetry breaking in ScV6Sn6, and the comparison to KV3Sb5.

From: Nanoscale visualization and spectral fingerprints of the charge order in ScV6Sn6 distinct from other kagome metals

Fig. 5

a Energy-dependent amplitudes of the three inequivalent CDW peaks (marked in the example Fourier transform in the inset) in ScV6Sn6. The overall shape of all three dispersion curves is nearly identical and largely overlaps one another. b Zoom-in on representative high-resolution dI/dV(r, V) maps showing the approximately rotationally symmetric real-space signature. c Energy-dependent amplitudes of the three inequivalent CDW peaks (marked in the example Fourier transform in the inset) in cousin kagome metal KV3Sb5. the dispersion of Qc amplitude is noticeably different than the other two, Qa and Qb, that are nearly indistinguishable. d Representative dI/dV(r, V) maps showing a unidirectional real-space signature that breaks the six-fold symmetry. STM setup conditions: (a) Iset = 30 pA, Vsample = -100 mV, Vexc = 5 mV; (b) Iset = 100 pA, Vsample = 100 mV, Vexc = 2 mV; (c, d) Iset = 150 pA, Vsample = 10 mV, Vexc = 1 mV. Scale bars correspond to: (b) 1 nm; (d) 4 nm.

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