Observation of periodic structures and pseudogaps in pristine compound α-TiNCl by STM/STS and break junction methods

Author:

Sugimoto Akira1ORCID,Matsumoto Kaito1,Saito Takeshi1,Yoshida Daiki1,Ekino Toshikazu1,Tanaka Masashi2,Gabovich Alexander M.3ORCID

Affiliation:

1. Graduate School of Advanced Science and Engineering, Hiroshima University 1 , Higashi-Hiroshima 739–8521, Japan

2. Department of Basic Science, Kyushu Institute of Technology 2 , Kitakyushu 804–8550, Japan

3. Institute of Physics, National Academy of Sciences of Ukraine 3 , Kyiv 03028, Ukraine

Abstract

Scanning tunneling microscopy and spectroscopy (STM/STS) and break-junction tunnel spectroscopy (B.TTS) measurements are performed on the pristine layered α-TiNCl semiconductor (pri-TiNCl), being the precursor of superconducting nitride chlorides. The STM topography of pri-TiNCl shows basic crystal structures with the lattice periods of a0≈ 0.38 nm and b0≈ 0.31 nm, ensuring that a clean a–b surface of micro-single crystals is obtained. From the STS measurements, the averaged conductance versus voltage dependence dI/dV(V) reveals kink structures at relatively high bias voltages of |F| ∼ −50 mV and −100 mV. The spatial (r-) conductance distributions dI/dV (V, r) (dI/dV maps) proportional to those of quasiparticle local densities of states (LDOSes) exhibit the bias-independent streak structures with the period of (4.8 ± 0.2) b0, which are predominantly observed within the range of |V| < 95 mV. The temperature dependence of the dI/dV B.TTS spectra shows the gap structure with the energy scale of 4Σ = 180 meV vanishing at Ts ∼ 120 K. Thus, the ratio of the gap Σ to the transition temperature Ts is 2Σ/kBTs ∼ 10. Here, kB is the Boltzmann constant. Such a ratio is typical of the pseudogap features in cuprate superconductors and dielectric gap characteristics in layered chalcogenides with charge-density waves.

Publisher

AIP Publishing

Subject

General Physics and Astronomy,Physics and Astronomy (miscellaneous)

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