Y. Ishimaru et al., SUPERCONDUCTING-GAP SYMMETRY STUDY USING A C BOUNDARY JOSEPHSON-JUNCTIONS IN YBA2CU3O7-DELTA FILMS/, Physical review. B, Condensed matter, 55(17), 1997, pp. 11851-11859
We have investigated gap symmetry of high-T-c superconductors using Jo
sephson junctions formed along a boundary of an a-axis-oriented YBa2Cu
3O7-delta (YBCO) grain surrounded by c-axis-oriented YBCO grains (a/c
boundary). There are two types of a/c boundary junctions; one is the b
oundary between (001) of a-axis-oriented grains and (100) of c-axis-or
iented grains, and the other is the boundary between (001) of a-axis-o
riented grains and (110) of c-axis-oriented grains. TEM observation sh
ows clean, sharp, and nearly single-facet interface along the grain bo
undaries in both types. In the case of the (100)-(001) type a/c bounda
ry junction, typical resistively shunted junction (RSJ)-type I-V curve
s, Shapiro steps under microwave irradiation, and Fraunhofer-like diff
raction pattern of I-c under magnetic field are observed, indicating t
hat the boundary works as a Josephson junction. In the case of the (11
0)-(001)-type a/c boundary junction, typical RSJ type I-V curves and S
hapiro steps under microwave irradiation are also observed. However, t
he diffraction pattern of I-c under magnetic field has the minimum val
ue at zero magnetic field. This property is analogous to one observed
for a corner junction which is formed between Pb and YBCO. These resul
ts show that the (110) of YBCO has a phase difference of pi and d(x)(2
)-(2)(y) superconducting-gap symmetry is in CuO2 planes of YBCO. But,
the (001) of YBCO has no phase difference of pi in spite of the existe
nce of d-wave symmetry in YBCO.