Asosiy kontentga oʻtish
AkademIndex

Mahsulotlar

Ishlab chiquvchilar uchun

AkademBaseEkotizim uchun ochiq API
Maqola

Peculiarities of pseudogap in Y0.95Pr0.05Ba2Cu3O7−δ single crystals under pressure up to 1.7 GPa

A. L. SolovjovB. Verkin Institute for Low Temperature Physics and Engineering, NAN of Ukraine, 47 Nauky Avenue, Kharkiv, 61103, UkraineL. V. OmelchenkoB. Verkin Institute for Low Temperature Physics and Engineering, NAN of Ukraine, 47 Nauky Avenue, Kharkiv, 61103, UkraineE. V. PetrenkoB. Verkin Institute for Low Temperature Physics and Engineering, NAN of Ukraine, 47 Nauky Avenue, Kharkiv, 61103, UkraineР. В. ВовкV. Karazin Kharkiv National University, 4 Svobody Square, Kharkiv, 61077, UkraineV. V. KhotkevychDiamond Light Source Ltd., Harwell Science and Innovation Campus, Didcot, OX11 0DE, United KingdomA. ChroneosDepartment of Materials, Imperial College, London, SW7 2AZ, UK. [email protected]
2019en
ABI

Annotatsiya

Abstract The effect of hydrostatic pressure up to P = 1.7 GPa on the fluctuation conductivity σ′(T) and pseudogap ∆*(T) in Y 0.95 Pr 0.05 Ba 2 Cu 3 O 7−δ single crystal with critical temperature Т с = 85.2 K (at P = 0) was investigated. The application of pressure leads to the increase in T c with dT c /dP = +1.82 K∙GPa −1 while the resistance decreases as dlnρ(100 K)/dP = −(10.5 ± 0.2) %∙GPa −1 . Regardless of the pressure, in the temperature interval from T c to T 0 (~88 K at P = 0) the behaviour of σ′(T) is well described by the Aslamazov – Larkin (AL – 3D) fluctuation theory, and above the T 0 by the Lawrence – Doniach theory (LD). The Maki-Thompson (MT – 2D) fluctuation contribution is not observed. This indicates the presence of structural defects in the sample induced by Pr. Here it is determined for the first time that when the pressure is applied to the Y 1−x Pr x Ba 2 Cu 3 O 7−δ single crystal, the pseudogap increases as dlnΔ*/dP = 0.17 GPa –1 .

Hali tarjima qilinmagan

Identifikatorlar

Iqtiboslar va manbalar

2 ta iqtibos0 ta foydalanilgan manba