Investigating the normal state and superconducting state properties of orthorhombic and hexagonal ZrRuP: A first-principles study
S. Bağcı, M. Cin, H. Y. Uzunok, Ertuǧrul Karaca, H. M. Tütüncü, G. P. Srivastava
DOI 10.1103/PhysRevB.100.184507 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
We have executed ab initio pseudopotential calculations on the structural, electronic, elastic, mechanical, vibrational, and electron-phonon interaction properties of hexagonal ZrRuP (h-ZrRuP) and orthorhombic ZrRuP (o-ZrRuP). The electronic states of both phases near the Fermi energy are found to be dominated by the d electrons of transition metal atoms, suggesting that they play a more active role in the generation of superconducting state for both phases of ZrRuP. A critical assessment of their elastic and mechanical properties reveals that the lattice of h-ZrRuP is softer than that of o-ZrRuP. A comparison of phonon dispersion curves for both phases indicates that the lower transverse acoustic branch of h-ZrRuP is much softer than that of o-ZrRuP. The soft character of this phonon branch gives rise to strong electron-phonon interaction in h-ZrRuP. Therefore the electron-phonon coupling parameter for h-ZrRuP equals to 1.25 which is considerably larger than the corresponding value of 0.57 for o-ZrRuP. As a consequence, phonon and electron-phonon interaction properties are crucial in making superconducting transition temperature much higher for h-ZrRuP than o-ZrRuP. At the end, the value of this temperature is found to be 12.49 K for h-ZrRuP and 3.89 K for o-ZrRuP which coincide with their experimental values of 12.93 and 3.82 K.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| ZrRuP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12.49 | Pressure not reported | unknown |
| ZrRuP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.89 | Pressure not reported | unknown |
| ZrRuP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12.93 | Pressure not reported | unknown |
| ZrRuP Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.82 | Pressure not reported | unknown |
| ZrRuSi Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 12 | Pressure not reported | unknown |
Similar papers
Electronic structure of the superconducting compounds o-ZrRuP and MoRuP
similarity 0.95Izumi Hase
Source status unknown — claims are unverified
Superconductivity of ZrRuSi prepared at high pressure
similarity 0.95Ichimin Shirotani et al.
Source status unknown — claims are unverified
Electronic structure of superconducting compounds h−ZrRuX (X=P,As,Si)
similarity 0.94Izumi Hase
Source status unknown — claims are unverified
Probing the superconducting gap structure of ScRuSi via μSR and first-principles calculations
similarity 0.94K. Panda et al.
Source status unknown — claims are unverified
Probing the superconducting gap structure in the noncentrosymmetric topological superconductor ZrRuAs
similarity 0.94Debarchan Das et al.
Source status unknown — claims are unverified
Probing the superconducting ground state of ZrIrSi: A muon spin rotation and relaxation study
similarity 0.93K. Panda et al.
Source status unknown — claims are unverified