“…For small b it follows a power law and in the range 10 −4 ≤ b ≤ 0.005 is approximated as f = 0.5552 • b −0.537 with the accuracy of ±1.2%. The dependence J ∝ B −α with α 0.4-0.8 was often observed for YBa 2 Cu 3 O 7−δ films 10,12,19,21,23,52,64 and 2G-tapes. 9 As seen in Fig.…”
Section: Discussionmentioning
confidence: 73%
“…Due to strong demagnetization effect a self demagnetizing field is produced by current flowing in a superconducting film when field is applied perpendicular to the film plane. [50][51][52] In the critical state this self field exists even after complete removal of external field. The measurements were performed for applied fields of 910 and 1530 Oe and in self-field after removing field of 2090 Oe.…”
Section: Methodsmentioning
confidence: 99%
“…Combining M * with data on δM (t) we precisely obtained the time dependence of the magnetic moment M (t). 52,57 Examples of M (t) curves obtained at low and high temperatures are shown in Figure 1. As seen, the noise of the curves is considerably lower than the change of the moment due to relaxation.…”
Section: Methodsmentioning
confidence: 99%
“…Preliminary results of the relaxation experiments were published elsewhere. 52,57,58 In the present work we analyze the current obtained from the M * (T ) dependences so let us consider this issue in detail.…”
Combined action of weak and strong pinning centers on the vortex lattice complicates magnetic behavior of a superconductor since temperature and magnetic field differently affect weak and strong pinning. In this paper we show that contributions of weak and strong pinning into magnetization of the layered superconductor YBa2Cu3O 7−δ can be separated and analyzed individually. We performed a careful analysis of temperature behavior of the relaxed superconducting current J in YBa2Cu3O 7−δ films which revealed two components of the current J = J1 + J2. A simple method of separation of the components and their temperature dependence in low magnetic fields are discussed. We found that J1 is produced by weak collective pinning on the oxygen vacancies in CuO2 planes while J2 is caused by strong pinning on the Y2O3 precipitates. J1 component weakly changes with field and quasi-exponentially decays with temperature, disappearing at T 30-40 K. Rapid relaxation of J1 causes formation of the normalized relaxation rate peak at T 20 K. J2 component is suppressed by field as J2 ∝ B −0.54 and decays with temperature following to the power law J2 ∝ (1 − T /T dp ) α where T dp is the depinning temperature. Detailed comparison of the experimental data with pinning theories is presented.
“…For small b it follows a power law and in the range 10 −4 ≤ b ≤ 0.005 is approximated as f = 0.5552 • b −0.537 with the accuracy of ±1.2%. The dependence J ∝ B −α with α 0.4-0.8 was often observed for YBa 2 Cu 3 O 7−δ films 10,12,19,21,23,52,64 and 2G-tapes. 9 As seen in Fig.…”
Section: Discussionmentioning
confidence: 73%
“…Due to strong demagnetization effect a self demagnetizing field is produced by current flowing in a superconducting film when field is applied perpendicular to the film plane. [50][51][52] In the critical state this self field exists even after complete removal of external field. The measurements were performed for applied fields of 910 and 1530 Oe and in self-field after removing field of 2090 Oe.…”
Section: Methodsmentioning
confidence: 99%
“…Combining M * with data on δM (t) we precisely obtained the time dependence of the magnetic moment M (t). 52,57 Examples of M (t) curves obtained at low and high temperatures are shown in Figure 1. As seen, the noise of the curves is considerably lower than the change of the moment due to relaxation.…”
Section: Methodsmentioning
confidence: 99%
“…Preliminary results of the relaxation experiments were published elsewhere. 52,57,58 In the present work we analyze the current obtained from the M * (T ) dependences so let us consider this issue in detail.…”
Combined action of weak and strong pinning centers on the vortex lattice complicates magnetic behavior of a superconductor since temperature and magnetic field differently affect weak and strong pinning. In this paper we show that contributions of weak and strong pinning into magnetization of the layered superconductor YBa2Cu3O 7−δ can be separated and analyzed individually. We performed a careful analysis of temperature behavior of the relaxed superconducting current J in YBa2Cu3O 7−δ films which revealed two components of the current J = J1 + J2. A simple method of separation of the components and their temperature dependence in low magnetic fields are discussed. We found that J1 is produced by weak collective pinning on the oxygen vacancies in CuO2 planes while J2 is caused by strong pinning on the Y2O3 precipitates. J1 component weakly changes with field and quasi-exponentially decays with temperature, disappearing at T 30-40 K. Rapid relaxation of J1 causes formation of the normalized relaxation rate peak at T 20 K. J2 component is suppressed by field as J2 ∝ B −0.54 and decays with temperature following to the power law J2 ∝ (1 − T /T dp ) α where T dp is the depinning temperature. Detailed comparison of the experimental data with pinning theories is presented.
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