Magnetotransport behavior of YBa2Cu3O7-δ –Sm0.55Sr0.45MnO3 superconducting-ferromagnetic composite thin films

Author:

Kumari Suman,Anas Mohd,Raghav D S,Chauhan Shital,Siwach P K,Malik VivekORCID,Singh H KORCID

Abstract

Abstract We report a detailed study on the magnetotransport behavior of YBa2Cu3O7-δ -Sm0.55Sr0.45MnO3 (YBCO-SSMO) superconducting-ferromagnetic composite thin films (thickness ∼80 nm) of nominal compositions (YBCO)1-x(SSMO)x (x = 0, 0.08, and 0.14). Films are grown by pulsed laser deposition of the pure and composite targets on (001)-SrTiO3 substrates, and all are single crystalline with the c-axis normal to the plane of the substrate. The Tc(R = 0) of the pure YBCO film is ≈87 K and decreases to ≈75 K and ≈44 K with the incorporation and increase of the ferromagnetic fraction in the superconducting matrix. Successive decrease in the slope of the normal state R-T curves maps the incorporation of the high resistance channels of the SSMO. In an external magnetic field (H), the rate of decrement in the Tc(R = 0) is found to be dTc(R = 0)/dH ∼1.8 K T−1, ∼4.7 K T−1, and ∼2.8 K T−1, respectively for x = 0, 0.08, and 0.14. The upper critical field and the irreversibility field are appreciably depressed in the composite samples and suggest a broadening of the mixed-phase vortex regime. The application of the thermally activated flux flow (TAFF) model shows that the activation energy decreases sharply from U0 = 4314 (910) meV, 498 (130) meV, and 253 (66) meV for YS00, YS08, and YS14, respectively, at H = 0 T (6 T). The analysis of the field-dependent activation energy in terms of U 0 H α and U 0 U log H dependence suggests decoupling of the 2D vortices due to the ferromagnetic phase. The hysteresis in the current-voltage characteristics is seen to decrease with an increase in the SSMO content.

Funder

Dr. K.K. Maurya

INSPIRE

Department of Science and Technology

IIT Roorkee

CSIR

Publisher

IOP Publishing

Subject

Condensed Matter Physics,Mathematical Physics,Atomic and Molecular Physics, and Optics

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