2005
DOI: 10.1109/tasc.2005.849427
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Addition of alternate phase nanoparticle dispersions to enhance flux pinning of Y-Ba-Cu-O thin films

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Cited by 8 publications
(22 citation statements)
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“…Transition temperatures of multilayer {(211 $1.2 nm /123 $11 nm ) · N, N = 20-25} and 123-only samples were virtually the same $89-90 K measured at AFRL by ac susceptibility methods [16] and at ORNL by transport methods. This is slightly different from T c measurements on single crystals where a small decrease of $1-2 K was measured for similar multilayer compared to 123 films [15].…”
Section: Resultsmentioning
confidence: 53%
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“…Transition temperatures of multilayer {(211 $1.2 nm /123 $11 nm ) · N, N = 20-25} and 123-only samples were virtually the same $89-90 K measured at AFRL by ac susceptibility methods [16] and at ORNL by transport methods. This is slightly different from T c measurements on single crystals where a small decrease of $1-2 K was measured for similar multilayer compared to 123 films [15].…”
Section: Resultsmentioning
confidence: 53%
“…Buffered Ni 0.97 W 0.03 (Ni-W) substrates were prepared at Oak Ridge National Laboratory (ORNL) and American Superconductor Corporation (AMSC) using similar procedures [11], and buffered Ni substrates were prepared at Air Force Research Laboratory (AFRL) [16] [11,16]. Buffered Ni substrates were prepared with a cap layer of CeO 2 $70 nm thick, an intermediate layer of YSZ $500 nm thick, and a seed layer of CeO 2 $70 nm, using pulsed laser deposition (PLD) for all buffer layers [16].…”
Section: Methodsmentioning
confidence: 99%
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“…[2][3][4] Many methods of introducing defects can be considered to increase flux pinning in YBCO, [2][3][4] and recent efforts have studied the use of (M x /123 y ) N heterostructures to introduce~3 to 20 nm-size island-growth nanoparticles or even larger-diameter plate-like defects into the films. [5][6][7][8][9][10][11][12][13][14][15][16][17] A number of different second-phase additions M have been tested, including M = green-phase 211, 5-12 Y 2 O 3 , 11,12,14,15 CeO 2 , [11][12][13] IrZrO 3 , 16 BaZrO 3 , 17 and other phases with negative effects on T c and/or J c (H) including M = La211, 11,12 MgO, 11,12 and Sm123. 12 Studies of (M x /123 y ) N heterostructures can provide basic information about the relative pinning properties of different M phases, and specific parameters of flux pinning such as the effects of different layer spacings.…”
Section: Introductionmentioning
confidence: 99%
“…[5][6][7][8][9][10][11][12][13][14][15][16][17] This paper presents a systematic comparison of film properties for selected M phases and different x layer thickness. A significant result observed is that the surface coverage is an important constant factor to optimize flux pinning, regardless of the M phase.…”
Section: Introductionmentioning
confidence: 99%