On the causes of low critical current in twin film high-temperature superconductors

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Abstract

The influence of internal local and external demagnetization fields on the critical current density of inter-doublet Josephson weak bonds Jc of high-temperature superconducting YBCO samples is investigated using the oscillation differential technique of local approximation. In the zero-field and zero-field cooling with flux accumulation regimes for samples with different Jc and twin sizes d, the demagnetization fields of samples HD1 and HD2 have been measured. The values of: d; thermodynamic first critical magnetic fields of twins Hic1; twin demagnetization fields HD tr; density of intra-twin effective critical currents Jc ef; critical pinning currents Jc p and shielding Meissner critical currents Jc M are determined. It is shown that at Hic1 fields the twins of large sizes “disintegrate” into a group of smaller twins with close demagnetizing factors. It is found that an increase in Jc M, Jc ef, and a decrease in d lead, on the one hand, to a decrease in Jc due to an increase in the demagnetization field of the sample HD and HD tr created by Jc ef and Jc M, and, on the other hand, to an increase in Jc ef and Jc M due to a decrease in d.

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About the authors

Kh. R. Rostami

Kotelnikov Institute of Radioengineering and Electronics RAS

Author for correspondence.
Email: rostami@ms.ire.rssi.ru

Fryazino branch

Russian Federation, Vvedenskii Squar., 1, Fryazino, Moscow region, 141190

V. А. Luzanov

Kotelnikov Institute of Radioengineering and Electronics RAS

Email: rostami@ms.ire.rssi.ru

Fryazino branch

Russian Federation, Vvedenskii Squar., 1, Fryazino, Moscow region, 141190

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Supplementary files

Supplementary Files
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1. JATS XML
2. Fig. 1. Typical magnetic field dependences of demagnetization fields: a – two samples Нр (Нв), curves 1, 1′ – sample No. 1, curves 2, 2′ – sample No. 2, measured in the ZFC (1, 2) and ZFCMFA (1′, 2′) modes at T = 77.4 K; b – the difference between the curves shown in Fig. 1a: 1 and 2 (curve 1) and 1′ and 2′ (curve 2). Temperature T = 77.4 K.

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3. Fig. 2. Dependences Jc М (1/d) at temperature T = = 77.4 K. Solid squares – sample No. 1, light squares – sample No. 2.

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4. Fig. 3. Distribution diagram of demagnetization fields.

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5. Fig. 4. Dependences of the effective critical current of twins: (a) – Jc eff (Jc M); (b) – Jc eff (1/d). Curves 1 correspond to sample No. 1, curves 2 – to sample No. 2. Temperature T = 77.4 K.

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6. Fig. 5. Dependences of the difference in the density of critical currents Jc and Jc eff, measured using the four-probe scheme and magnetic measurements, respectively: (a) – (Jc – Jc eff) (Hтк1); (b) – (Jc – Jc eff) (Jc M); (c) – (Jc – Jc eff) (1/d). Curve 1 corresponds to sample No. 1, curve 2 – to sample No. 2. Temperature T = 77.4 K.  

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