Structural distortion and suppression of superconductivity in stoichiometric B1−MoN epitaxial thin films
Kei Inumaru, Kazuya Baba, Shoji Yamanaka
DOI 10.1103/PhysRevB.73.052504 · Physical Review B
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Abstract
Molybdenum nitride films with the NaCl structure (B1−MoN) were epitaxially grown on α−Al2O3(001) and MgO(001) substrates at 973K by pulsed laser deposition (PLD) under nitrogen radical irradiation. The highly crystalline epitaxial films enabled us to determine the three-dimensional cell parameters, which was motivated by theoretical calculations that B1−MoN, a predicted superconductor, is elastically unstable against tetragonal and trigonal distortions. On α−Al2O3(001), the B1−MoN phase (composition, Mo1N0.98) was grown with its (111) planes parallel to the substrate surface. X-ray diffraction analysis with a multiaxes diffractometer detected only a small trigonal lattice distortion [a=0.4219(3)nm, α=89.28(5)°] with an expansion along the [111] direction perpendicular to the substrate surface. The film grown on MgO(001) had the MoN1.03 composition and showed a slight tetragonal distortion (a=0.4213 and c=0.424nm) due to fitting to the MgO substrate lattice (a=0.4213nm). These two stoichiometric films showed no superconductivity above 2K. A lower nitrogen content (MoN0.86) film was obtained on α−Al2O3(001) using a higher deposition rate. The corresponding film had a much smaller lattice constant [a=0.4184(3)nm], and a similar distortion [α=89.41(5)°]. The B1−MoN0.86 film showed superconductivity with a transition temperature Tc=4.2K. The suppression of the superconductivity of the former stoichiometric phase can be interpreted in terms of the lattice expansion.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| MoN0.86 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.2 | Pressure not reported | onset |
| MoN0.98 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| MoN1.03 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| γ-Mo2N Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5 | Pressure not reported | unknown |
| β-Mo2N Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5 | Pressure not reported | unknown |
| δ-MoN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12 | 6 GPa | unknown |
| MoN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 29 | Pressure not reported | unknown |
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