Magnetization hysteresis loops (MHL) were measured on two NEG-123 bulk samp
les with addition of 30% Gd-211 fine (sub-micron) particles in the temperat
ure range 65-88 K. These two samples possessed significantly different seco
nd-to-central peak heights ratios, Both sets of the J(c)-B curves could be,
however, fitted with a high precision by the same combined analytical func
tion J(c)(B) = J(cp) exp(-alphaB/B-p) + J(sp)b(p) exp[(1 - (B/B-p)(n))/n] i
n all investigated temperatures. The pinning regimes governing formation of
the central and second peak could be separated in this way. As far as the
central peak contribution to the MHL becomes usually negligible at around B
-p, the shape of J(c)(B) above B-p is governed by only a high-field pinning
mechanism. The central peak extends to this field region only at temperatu
res very close to T-c. Good scaling of the pinning force density with tempe
rature gives a further support to the above conclusions. (C) 2001 Elsevier
Science B.V. All rights reserved.