1965
DOI: 10.1016/0038-1098(65)90285-1
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Direct evidence for quantized flux threads in type - II superconductors

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Cited by 35 publications
(13 citation statements)
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“…[1][2][3] Tuning the external applied magnetic field one can switch between rich varieties of energetically favorable or metastable vortex configurations, which cannot be realized in bulk systems. Of particular interest is a possibility to obtain multiquanta ͑giant͒ vortex states with winding numbers larger than unity for certain intervals of external magnetic field ͑see, e.g., Ref.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3] Tuning the external applied magnetic field one can switch between rich varieties of energetically favorable or metastable vortex configurations, which cannot be realized in bulk systems. Of particular interest is a possibility to obtain multiquanta ͑giant͒ vortex states with winding numbers larger than unity for certain intervals of external magnetic field ͑see, e.g., Ref.…”
Section: Introductionmentioning
confidence: 99%
“…This value is approximately one order of magnitude higher than the time for the single-vortex creation. This was measured for the first time by G. Boato, G.Gallinaro and C. Rizzuto [28], who showed that this time is less than 10 −5 s.…”
Section: Resultsmentioning
confidence: 99%
“…͑21͒ in more detail. Within the standard quasiclassical approximation ͑assuming k r ӷ1) this solution can be written in the form ͑we take the equation for ⌿ ϩ for definiteness͒ ⌿ ϩ ϭg 1 (r)H (1) (k r r) ϩg 2 (r)H (2) (k r r), where H (1,2) (k r r) are Hankel functions and g 1,2 are slowly varing envelopes. Far from the normal metal cylinder (rӷa,⌬ϭconst) we have the two exact solutions H (1,2)…”
Section: ͑20͒mentioning
confidence: 99%
“…Ϫ2ik F /). Inside the normal metal cylinder (⌬ϭ0) there are also two exact solutions H (1,2) (k r r). To avoid a divergence of the wave function for r→0 we must match the two independent solutions at the origin and obtain Bessel function for small r. One can see that for nonzero imaginary part of the wave vector ͱk r 2…”
Section: ͑20͒mentioning
confidence: 99%