Reentrant Softening in Copper-Oxide Superconductors (original) (raw)

Elastic properties of superconducting and non-superconducting DyBaSrCu3O7−δ

Physics Letters A, 2001

Ultrasonic longitudinal and shear wave velocities were measured for superconducting and non-superconducting DyBaSr Cu 3 O 7−δ (Dy-1113) at 10 MHz between 80 and 270 K. The superconducting sample exhibits a step-like elastic anomaly between 190 and 230 K. No elastic anomaly was observed in the non-superconducting Dy-1113. The anomaly observed in the superconducting sample is attributed to structural phase transition caused by oxygen orderings.

Superconductivity and Elastic Properties of La1.85-1.5xSr0.15+1.5xCu1-xMnxO4 with x = 0, 0.02 and 0.04

Sains Malaysiana, 2018

The effects of mixed-valence Mn substitution at the Cu site on the superconducting and elastic properties of La 1.85-1.5x Sr 0.15+1.5x Cu 1-x Mn x O 4 (x = 0, 0.02 and 0.04) were studied. The samples were characterized by X-ray diffraction (XRD) method, temperature-dependent resistance measurements, scanning electron microscopy (SEM) and sound velocity measurements at room temperature. An elastic softening and a decrease in the critical temperature T c was observed as Mn was substituted for Cu. The Debye temperature θ D for x = 0 and 0.02 void free samples were calculated to be 459 K and 430 K, respectively. Internal lattice strain which is related to lattice parameter ratio a/c did not correlate with T c. The electron-phonon coupling estimated using the conventional Bardeen-Cooper-Schrieffer (BCS) theory was λ = 0.367 (x = 0) and 0.368 (x = 0.02). The electron-phonon coupling in two-dimensional van Hove scenario was calculated to be λ vH = 0.0148 (x = 0) and 0.0149 (x = 0.02). These results were compared with other cuprates and related superconductors. The comparison showed that other than electron-phonon coupling, the elastic moduli might play an important role in the mechanism of superconductivity in these materials.

Anisotropy of Elastic and Relaxation Properties of the Superconducting 123-YBCO Single Crystal

Le Journal de Physique IV, 1996

Acoustic properties of the YBazCu306.7 sjngle rystal are studied in the temperature range 5-300 K. The wave vector of the longitudinal and torsional/Standing waves in the frequency range 50-90 kHz was diwcted along and normal to the c-axis. It is showm that the acoustic anomalies observed in the single crystal qualitatively are the same that those found earper in t h k l 2 3-~~~0 ceramics but depend strongly on the mutual orientation of the wave vector and the c-&xis. It is1established that the significant temperature hysteresis and "softening" of the dynamic elastic moduli at thermocycling are observed only in the case when the sound waves have a displacement component along the c-axis. Moreover, in this case the sound absorption peak near 230 K is more pronounced. The locations ofjsound absorption peaks are not sensitive to the oscillation mode and sample orientation. The results obtaiqed are qualitatively consistent with the model of bistable behaviour of the sublattice formed by apical oxygkn .atoms.

Softening of Cu-O vibrational modes as a precursor to onset of superconductivity inEuBa2Cu3O7−δ

Physical Review B, 1988

TMependent "Sn Mossbauer Debye-Wailer factors f(T) in EuBa2Cu2. 9sSnvm07 s display evidence of a substantial softening in lattice vibrations at T &110 K. In a previous ' 'Eu study, no detectable softemng in f(T) was found at the rare-earth site. These results taken together show that Sn atoms as a dilute impurity replace predominantly Cu(1) sites in the Cu-0 chains of the orthorhombic structure. It appears that a softening in vibrational modes localized onto the Cu-0 linear chains occurs as a precursor to the onset of superconductivity. These results show that phonons do appear to play an important role in electron pairing in these high-T, oxide superconductors.

Anomalous breaking of phonon softening in the superconducting state of La1.85Sr0.15CuO4

Physica C: Superconductivity, 1996

Neutron inelastic scattering measurements on single crystals of La2_xSrxCuO4_y have been performed to study the relation between the soft phonon and the superconductivity. The phonon softening of the Z-point mode due to the incipient structural phase transition to the low-temperature tetragonal (P42/ncm) or orthorhombic (Pccn) phase appeared to be frozen below T c. The narrowing of the phonon line-width upon cooling was saturated below T c, suggesting the appearance of the extra line broadening in the superconducting state.

Bond Stretching Phonon Softening of Underdoped Copper-Oxide Superconductors

Journal of Superconductivity and Novel Magnetism, 2012

The anomalous properties of the bond stretching (BS) phonon mode are analyzed in the underdoped region of cuprates by studying the t-t -J -Holstein model and the Hubbard-Holstein model with both numerical and analytical approaches. It is shown that a BS phonon softening occurs at an intermediate wavevector along the horizontal direction of the Brillouin zone (BZ) in agreement with recent INXS experiments as the result of the interaction among strongly correlated holes and antiferromagnetic fluctuations. An explanation of the single vs. double mode scenario is also discussed.

Superconductivity and Phonon Softening

Physical Review Letters, 1972

A new formula is derived which relates changes in electron-phonon coupling strength A, to shifts in phonon frequencies. Using this formula, the superconducting transition temperature T~is discussed for bce transition metals and rock-salt-structure transition-metal carbides. Among superconducting elements and compounds, it is common to find pairs of metals with the same crystal structure, made of elements in neighboring columns of the periodic table, in which the transition temperature T, differs greatly. Good examples are the rock-salt-structure materials HfC (with T, & 0.015'K) and TaC (with T,-11'K). Recently Smith and 615,ser' and Smith' have re