1994
DOI: 10.2172/79036
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Origin of 1/f noise peaks of YBa{sub 2}Cu{sub 3}O{sub x} films in a magnetic field

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“…As observed experimentally, there is a strong difference in the noises generated in stationary and non stationary conditions. When a constant current is flowing in a HTSC made resistive by a d.c. magnetic field (or by the current itself when it is sufficiently large) a current noise is generated whose power spectrum is of the 1/f type [2,3,4,5,6], while when the current or the field are changing an additional noise component occurs whose power spectrum is of the 1/f 2 type [7]. This component dominates the low frequency part of the power spectrum, and, in the case of the magnetic field variation, it is so large that the 1/f component is negligible and the whole spectrum appears to be of the 1/f 2 type.…”
Section: Introductionmentioning
confidence: 99%
“…As observed experimentally, there is a strong difference in the noises generated in stationary and non stationary conditions. When a constant current is flowing in a HTSC made resistive by a d.c. magnetic field (or by the current itself when it is sufficiently large) a current noise is generated whose power spectrum is of the 1/f type [2,3,4,5,6], while when the current or the field are changing an additional noise component occurs whose power spectrum is of the 1/f 2 type [7]. This component dominates the low frequency part of the power spectrum, and, in the case of the magnetic field variation, it is so large that the 1/f component is negligible and the whole spectrum appears to be of the 1/f 2 type.…”
Section: Introductionmentioning
confidence: 99%