2009
DOI: 10.1016/j.physc.2009.01.012
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Influences of cooling height and lateral moving speed on the levitation characteristics of YBaCuO bulks

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Cited by 18 publications
(7 citation statements)
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“…This linear dependence, the very low value of emitted power and the width of the radiation peak all indicate that self-emission from the series array was incoherent. Published experiments on underdamped junction arrays [16,17] and their theoretical interpretation [18,19], as well as the recently presented model [20] for arrays of overdamped junctions (our case), suggest a threshold in the number of biased junctions embedded within a resonant cavity. This threshold must be exceeded to attain coherent self-emission.…”
Section: Resultsmentioning
confidence: 59%
“…This linear dependence, the very low value of emitted power and the width of the radiation peak all indicate that self-emission from the series array was incoherent. Published experiments on underdamped junction arrays [16,17] and their theoretical interpretation [18,19], as well as the recently presented model [20] for arrays of overdamped junctions (our case), suggest a threshold in the number of biased junctions embedded within a resonant cavity. This threshold must be exceeded to attain coherent self-emission.…”
Section: Resultsmentioning
confidence: 59%
“…Considering the sloping steps shown in figure 7 curve (a), the low value of the self-radiation power and the large width of the radiation peak, we infer that the self-radiation of the junction array was incoherent [1]. Previous research results, including experiments [21][22][23] and theories [24][25][26], have suggested a threshold in the number of biased junctions embedded in a resonant cavity. This threshold must be exceeded to attain coherent self-radiation.…”
Section: Experiments Results and Discussionmentioning
confidence: 74%
“…When the Josephson frequency w J equal to the resonance frequency of the circuit w rc , the oscillations in Josephson junction are tuned to this frequency. This resonance could manifested itself in the current-voltage characteristic (IV-characteristic) in a variety of ways; such as, steps [5,6], or humps and dips [7,8]. LC-shunting leads to a step in the one loop IV-characteristics, when the value of Josephson frequency approaches that of the resonance circuit.…”
Section: Introductionmentioning
confidence: 99%