The hole concentration p(␦), the transition temperature T c , the intragrain penetration depth , and the Meissner effect were measured for annealed RuSr 2 (Gd,Ce) 2 Cu 2 O 10ϩ␦ samples. The intragrain superconducting transition temperature T c varied from 17 to 40 K while the p changed by only 0.03 holes/CuO 2 . The intragrain superfluid density 1/ 2 and the diamagnetic drop of the field-cooled magnetization across T c ͑the Meissner effect͒, however, increased more than 10 times. All of these findings are in disagreement with both the T c vs p and the T c vs 1/ 2 correlations proposed for homogeneous cuprates, but are in line with a possible phase separation and the granularity associated with it. underdoped nature ͑i.e., the hole concentration pӶ0.16 holes/CuO 2 ) or the competition between the SC and the coexisting FM through the Fulde-FerrellLarkin-Ovchinnikov ͑FFLO͒ phase. 1-5 A verification was difficult until the recent reports that the transition temperatures T c of Ru1222 and Ru1212 can be adjusted over a broad range by oxygen annealing and Cu substitution, respectively. [6][7][8] The reported data, unfortunately, show that the T c enhancement is accompanied by both a p increase and a suppression of the ferromagnetic spin order and offer no clear distinction. To explore the topic, we measured the intragrain T c , the p, the intragrain superfluid density 1/ 2 , and the Meissner effect in several annealed Ru1222 samples. The data were then compared with both the T c vs p correlation 9 and the T c vs 1/ 2 line proposed. 10 We observed that a twofold enhancement of T c ͑from 17 to 40 K͒ is accompanied by a relatively small change of p ͑from 0.09 to 0.12 holes/CuO 2 ), but a 20-fold increase in 1/ 2 ͑from 0.3 to 6 m Ϫ2 ). Together with an extremely large field effect of dT c /dHϾ100 K/T and a linear increase of the Meissner fraction with 1/ 2 , the data suggest that those ruthenocuprate grains are actually Josephson-junction arrays ͑JJA's͒, in agreement with the phase-separation model suggested. 11 Further investigations of local magnetic structures are needed to solve the problem.Ceramic RuSr 2 (Gd 0.7 Ce 0.3 ) 2 Cu 2 O 10ϩ␦ samples were synthesized following the standard solid-state-reaction procedure. Precursors were first prepared by calcined commercial oxides at 400-900°C under flowing O 2 . Mixed powder with a proper cation ratio was then pressed into pellets and sintered at 900°C in air for 24 h. The final heat treatment of the ceramics was done at 1090°C for 60 h after repeatedly sintering and regrinding at 1000°C. Powders with different particle sizes were prepared according to the procedures previously reported. 12 The structure of the samples was determined by powder x-ray diffraction ͑XRD͒, using a Rigaku DMAX-IIIB diffractometer. The XRD pattern of a typical sample is shown in Fig. 1. Refinement was done based on a space group of I4/mmm with lattice parameters of aϭ3.839(1) and cϭ28.591(5) using the RIETAN-2000 program. 13 There are no noticeable impurity lines in the x-ray diffraction pattern ...