Summary
of Research Activity
As
a probe of the material properties, a microwave measurement is a useful
complement to low frequency susceptibility and resistivity measurements for at
least two reasons.
Firstly, it is contact less measurement. Secondly, it permits the study of the
resistive behavior below
super conducting
transition temperature
Tc . Additionally,
the changes in the micro structure of the materials are reflected in
the low field dependent microwave
absorption (LFDMA).
We
prepared the polycrystalline samples YBaCuO by
different methods and characterized them by resistivity measurements,
XRD, EPR and SEM. LFDMA was
studied in details in these well characterized
samples as a function of temperature, modulation field, microwave power
and grain size. All HTCS give intense LFDMA at and below Tc.
The derivative signal of LFDMA shows peak and hysteresis. Peak position (Hm ) of derivative signal of
LFDMA gives the measure of grain size of HTSC materials.
The
LFDMA signal arises due to the microwave loss in weak links forming
Josephson junctions
in granular
superconductors. In polycrystalline samples
there are
a large
number of
inter-granular Josephson junctions (JJ) of different sizes and oriented
randomly. All these
junctions can be
approximated by a single representative resistively shunted JJ. Microwave loss
was calculated in the single representative JJ on the basis of the RSJ model.
The calculated results agree with that of the experimental results
qualitatively. From this we conclude that microwave loss in the
polycrystalline samples is due to the intergranular JJ.
We
have also studied the field cooling (FC) and field exposure
(FE) effect on the LFDMA in
YBaCuO & TlBaCaCuO. The measurement of hysteresis area under field
cooling and field exposure gives the measure of lower critical field of inter granular junction (Hc1j ) and
that of grain (Hc1g ). From above
measurements it
has been
concluded that TlBaCaCuO have lower pinning force than YBaCuO. Thus the
above measurements gives the measure of relative pinning strength of the
materials.
We have also measured the resistivity and ac susceptibility of Zn doped LaBaCaCu3O7-d systems having Zn content of .5%, 1.0%, !.5%,2.0%, 2.5% and 3.0% at wt. From above studies following conclusions have been drawn about the role of Zn in LBCCO samples. (1) The conduction mechanism of electrons appears to follow a crossover from the purely metallic regime to localization regime due to either weak localization or electron-electron interaction effects after about 1.5% Zn. (2) The superconducting transition as revealed by resistivity vs temperature curves or susceptibility vs temperature curves becomes sharper with zn-content