1992
DOI: 10.2172/10188570
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Defect cascades produced by neutron irradiation in YBa{sub 2}Cu{sub 3}O{sub 7{minus}{delta}}

Abstract: by a Contrauor of the US. Government under contract No. W-31-109-ENG-38. Aaordingiy. the U.S. Oovernmenl retain8 a nonexclusive. royalty-lree Ikanse to Wish or reproduce the published lorm of thm contr0utbn. or albw DISCLAIMER This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thsreof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the… Show more

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Cited by 2 publications
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“…MeV) and they produce spherical defects of amorphous material with a diameter of a few nm (so called collision cascades) [15,[17][18][19]. The point defects and clusters of point defects are created by neutrons with lower energies and they can act as effective pinning as well [34].…”
Section: Tapes In High Magnetic Fields and After Irradiationmentioning
confidence: 99%
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“…MeV) and they produce spherical defects of amorphous material with a diameter of a few nm (so called collision cascades) [15,[17][18][19]. The point defects and clusters of point defects are created by neutrons with lower energies and they can act as effective pinning as well [34].…”
Section: Tapes In High Magnetic Fields and After Irradiationmentioning
confidence: 99%
“…Measurements of n-values after introducing additional pinning centres require special attention. Irradiation by fast neutrons introduces randomly distributed spherical pinning centres with diameters of a few nm [15][16][17][18][19][20] into a superconductor. It is a proven method of introducing efficient pinning centres into HTS, resulting in critical currents enhancements.…”
Section: Introductionmentioning
confidence: 99%
“…Fast neutrons (E > 0.1 MeV) generate collision cascades in cuprates by transferring sufficient energy to a primary knock-on atom, which initiates further collisions [15] [16]. These collisions lead to local melting of the lattice and the formation of spherical defects with a diameter of ≈ 6 nm [15]. The size of these normal conducting impurities matches the size of a flux line core (2ξ a,b ≈ 6 nm at 77 K) and is, therefore, optimal for flux pinning.…”
Section: Introductionmentioning
confidence: 99%
“…Fast neutrons (E > 0.1 MeV) generate collision cascades in cuprates by transferring sufficient energy to a primary knock-on atom, which initiates further collisions [15] [16]. These collisions lead to local melting of the lattice and the formation of spherical defects with a diameter of ≈ 6 nm [15].…”
Section: Introductionmentioning
confidence: 99%
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