2001
DOI: 10.1016/s0921-4534(00)01567-7
|View full text |Cite
|
Sign up to set email alerts
|

AC susceptibility of high Tc superconductor Tl0.8Pb0.2Bi0.2Sr1.6Ba0.4Ca2Cu3Ox using a critical state model

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
6
0

Year Published

2003
2003
2014
2014

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 23 publications
(6 citation statements)
references
References 19 publications
0
6
0
Order By: Relevance
“…In particular the loss component of the AC susceptibility has been used widely to probe the nature of weak links in polycrystalline superconductors. It is also employed to estimate some of the important physical properties like critical current density Jc and effective volume fraction of the superconducting grains [10][11][12][13]. Several critical state models have been very successful in accounting for major features of the temperature and field variation of AC susceptibility [14][15][16].…”
Section: Resultsmentioning
confidence: 99%
“…In particular the loss component of the AC susceptibility has been used widely to probe the nature of weak links in polycrystalline superconductors. It is also employed to estimate some of the important physical properties like critical current density Jc and effective volume fraction of the superconducting grains [10][11][12][13]. Several critical state models have been very successful in accounting for major features of the temperature and field variation of AC susceptibility [14][15][16].…”
Section: Resultsmentioning
confidence: 99%
“…It is also employed to estimate some of the important physical parameters like critical current density, J c , and effective volume fraction of the superconducting grains, f g . [28][29][30][31][32][33] Experimentally, the real part of AC susceptibility, 0 , in polycrystalline samples shows two drops as the temperature is lowered below onset of diamagnetic transition and correspondingly the derivative of the 0 ðTÞ displays two peaks. The first sharp drop at T c is due to the transition within grains and the second gradual change at T cJ is due to the occurrence of the weak link network between grains.…”
Section: Characterization Of Sintered Samplesmentioning
confidence: 99%
“…The first sharp drop at T c is due to the transition within grains and the second gradual change at T cJ is due to the occurrence of the weak link network between grains. [34][35][36] The imaginary part, 00 , shows a peak which is the sign of the dissipation in the sample.…”
Section: Characterization Of Sintered Samplesmentioning
confidence: 99%
“…As it is evident from this picture, there are two distinctive regions. Namely, above h = 15Oe the curves exhibit almost linear dependence which can be attributed to establishment of the well-documented [18,19,20,21] Bean type critical state regime with 1+4πχ ′ B (h) = 2h/J C D where J C is the fieldindependent critical current density and D the sample's thickness. On the other hand, below h = 15Oe, practically temperature-independent periodic oscillations are clearly seen.…”
Section: Resultsmentioning
confidence: 86%