Effect of Electromagnetic Interactions on the Undulatory Temperature Dependent Behaviour of Non-Resonant Microwave Absorption Signal Amplitude in Bi2Sr2CaCu2O8+x
スポンサーリンク
概要
- 論文の詳細を見る
Variation of non-resonant microwave absorption (NRMA) signal amplitude in single-phase Bi-2212 (5 wt % Ag) sintered pellets ($T_{\text{c}}^{\circ} \sim 96$ K) while increasing temperature from 15 to 105 K has been investigated and discussed. These studies show an undulatory behavior of an initial fall in the amplitude (15–71.8 K) with a subsequent narrow weak temperature independent region (71.8–75.6 K) and then a rise peaking at ${\sim}82.5$ K followed by a final exponential fall (82.5–105 K). A detailed discussion on earlier reported data has suggested that this undulatory behavior cannot be understood in terms of existing approaches involving effect of Josephson interactions (JI) alone among vortices. In our opinion, the entire undulatory behavior observed in the present samples can be explained with the inclusion of electromagnetic interaction (EMI) along with JI.
- Published by the Japan Society of Applied Physics through the Institute of Pure and Applied Physicsの論文
- 2006-01-15
著者
-
Das Bijoy
C-met
-
Sharma Mukul
National Physical Laboratory
-
Ekbote Shrikant
National Physical Laboratory
-
Padam Gursharan
National Physical Laboratory
-
Srivastava Ganesh
Deartment of Physics and Astrophysics, University of Delhi, Delhi-110007, India
-
Tripathy Malay
Deartment of Physics and Astrophysics, University of Delhi, Delhi-110007, India
-
Sharma Mukul
National Physical Laboratory, New Delhi-110012, India
-
Ekbote Shrikant
National Physical Laboratory, New Delhi-110012, India
-
Das Bijoy
C-MET, Pashan Road, Pune; 400 008, India
関連論文
- Comparative Study of Effect of Initial Sintering in Rod/Tube Shape on $J_{\text{c}}$ and Fracture Strength of Bi-2223: 10 wt % Ag Bulk Rod Conductors
- Effect of Electromagnetic Interactions on the Undulatory Temperature Dependent Behaviour of Non-Resonant Microwave Absorption Signal Amplitude in Bi2Sr2CaCu2O8+x