2020
DOI: 10.35848/1347-4065/ab6f2b
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Strong flux pinning by columnar defects with directionally dependent morphologies in GdBCO-coated conductors irradiated with 80 MeV Xe ions

Abstract: We show that Xe ion irradiation with 80 MeV to GdBa2Cu3Oy-coated conductors creates different morphologies of columnar defects (CDs) depending on the irradiation angles θi relative to the c-axis: continuous CDs with a larger diameter are formed for oblique irradiation at θi = 45°, whereas the same ion beam at a different angle (θi = 0°) induces the formation of discontinuous CDs. The direction-dependent morphologies of CDs significantly affect the angular behavior of the critical current density Jc. In particu… Show more

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Cited by 7 publications
(9 citation statements)
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“…The angular dependence of the double irradiated sample at ±30° can be fitted by three Lorentzian 3) give a combined effect to give a single strong and broad peak at ~15° and ~150°. This is expected since ±30° irradiated defects are oriented closer to c-axis peaks, giving a combined benefit to angles closer to the c-axis peaks and aligning with the results of studies on inclined angle irradiations [140][141] [190]. As in single 30° irradiation, the Gaussian components are not observed, which is masked by the strong and broad Lorentzian components due to the irradiated defects at ±30° indicating the dominancy of pinning by irradiated defects over the pinning benefit by defects with weak c-axis bias present in the pristine sample.…”
Section: Maximum Entropy Model Fitssupporting
confidence: 70%
“…The angular dependence of the double irradiated sample at ±30° can be fitted by three Lorentzian 3) give a combined effect to give a single strong and broad peak at ~15° and ~150°. This is expected since ±30° irradiated defects are oriented closer to c-axis peaks, giving a combined benefit to angles closer to the c-axis peaks and aligning with the results of studies on inclined angle irradiations [140][141] [190]. As in single 30° irradiation, the Gaussian components are not observed, which is masked by the strong and broad Lorentzian components due to the irradiated defects at ±30° indicating the dominancy of pinning by irradiated defects over the pinning benefit by defects with weak c-axis bias present in the pristine sample.…”
Section: Maximum Entropy Model Fitssupporting
confidence: 70%
“…27) Therefore, the present results are remarkable in finding that c-axis-directed 1D pins are effective for enhancing J c sf values at 77 K of YBCO, not only in the 100 kA cm −2 -order of bulk samples but also in the MA cm −2 -order of film samples. It is worth noting that in YBCO films and related materials, J c at 77 K in applied magnetic fields has been enhanced by continuous 11) and/or discontinuous 26,28) 1D irradiation defects in the order of 100 kA cm −2 .…”
Section: Resultsmentioning
confidence: 99%
“…The ion irradiation is a useful tool to generate the desired defect structure. Depending on the ion species, ion energy and the properties of the target materials, ion irradiation enables the creation of defects with well-controlled morphology and density, such as point [8], cluster [9][10][11][12] and columnar [13][14][15] defects. Early works on the ion irradiation of cuprate (Cu-O based) high-T c superconductors (HTS) for improving J c in the magnetic field have mostly focused on the high-energy, over hundreds of MeV, heavy ion irradiation [13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Depending on the ion species, ion energy and the properties of the target materials, ion irradiation enables the creation of defects with well-controlled morphology and density, such as point [8], cluster [9][10][11][12] and columnar [13][14][15] defects. Early works on the ion irradiation of cuprate (Cu-O based) high-T c superconductors (HTS) for improving J c in the magnetic field have mostly focused on the high-energy, over hundreds of MeV, heavy ion irradiation [13][14][15]. At this energy range, the irradiation of superconducting materials by the swift heavy ion mainly causes electronic excitation and ionization of the target atoms.…”
Section: Introductionmentioning
confidence: 99%