TY - JOUR
T1 - Investigation of the magnetic field-induced microwave absorption across Tc in single crystals of YBa2Cu3O7-δ and BiSrCaCuO. Anisotropy and magnetic field dependence
AU - Shaltiel, D.
AU - Ginodman, V.
AU - Golosovsky, M.
AU - Katz, U.
AU - Boasson, H.
AU - Gerhouser, W.
AU - Fischer, P.
PY - 1992/11/15
Y1 - 1992/11/15
N2 - The magnetic field-modulated microwave absorption near Tc has been studied in high-quality single crystals of YBa2Cu3O7-x (Tc ≈ 90 K) and in BiSrCaCuO (Tc ≈ 85 K) as a function of magnetic field B < 1.3 T and orientation. Sharp microwave absorption peaks were observed when sweeping the temperature through Tc from above. The analysis of the peaks using Tinkham's model for fluxon losses gives values for the pinning strength of A ≈ 1000 T and A ≈ 3 T for the YBaCuO and BSCCO crystals, respectively. The anisotropy values obtained from the orientation dependence of the peaks were ε{lunate} = 5 and ε{lunate} = 40-60 for these two compounds, respectively. The results are also discussed with respect to the B-T vortex phase diagram. A marked difference between the YBaCuO and BSCCO compounds is the presence of a low-temperature absorption signal with a different orientation dependence, observed only in the BSCCO compound, in addition to the signals just below Tc observed in both compounds.
AB - The magnetic field-modulated microwave absorption near Tc has been studied in high-quality single crystals of YBa2Cu3O7-x (Tc ≈ 90 K) and in BiSrCaCuO (Tc ≈ 85 K) as a function of magnetic field B < 1.3 T and orientation. Sharp microwave absorption peaks were observed when sweeping the temperature through Tc from above. The analysis of the peaks using Tinkham's model for fluxon losses gives values for the pinning strength of A ≈ 1000 T and A ≈ 3 T for the YBaCuO and BSCCO crystals, respectively. The anisotropy values obtained from the orientation dependence of the peaks were ε{lunate} = 5 and ε{lunate} = 40-60 for these two compounds, respectively. The results are also discussed with respect to the B-T vortex phase diagram. A marked difference between the YBaCuO and BSCCO compounds is the presence of a low-temperature absorption signal with a different orientation dependence, observed only in the BSCCO compound, in addition to the signals just below Tc observed in both compounds.
UR - http://www.scopus.com/inward/record.url?scp=0026949429&partnerID=8YFLogxK
U2 - 10.1016/0921-4534(92)90175-C
DO - 10.1016/0921-4534(92)90175-C
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AN - SCOPUS:0026949429
SN - 0921-4534
VL - 202
SP - 303
EP - 320
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 3-4
ER -