1971
DOI: 10.1016/0031-8914(71)90312-0
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Ultrasonic attenuation in superconducting molybdenum-rhenium alloys

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Cited by 7 publications
(2 citation statements)
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“…which is also used to determine the upper critical field at zero temperature [21]. For the sample MR6 the BCS coherence length ξ 0 is found to be 70 nm from the relation ξ 0 = v F /π∆(0) where v F = 5 × 10 5 m/s is the Fermi velocity [22] and ∆(0) = 1.8k B T c [23] is the BCS superconducting gap at zero temperature. Finally the mean free path has been estimated to be 3 nm from the measured low temperature resistivity ρ 10 K (expressed in µΩ cm), using the relation [24] = v 0 0.22…”
Section: Resultsmentioning
confidence: 99%
“…which is also used to determine the upper critical field at zero temperature [21]. For the sample MR6 the BCS coherence length ξ 0 is found to be 70 nm from the relation ξ 0 = v F /π∆(0) where v F = 5 × 10 5 m/s is the Fermi velocity [22] and ∆(0) = 1.8k B T c [23] is the BCS superconducting gap at zero temperature. Finally the mean free path has been estimated to be 3 nm from the measured low temperature resistivity ρ 10 K (expressed in µΩ cm), using the relation [24] = v 0 0.22…”
Section: Resultsmentioning
confidence: 99%
“…Rhenium is an exceptionally rare metal element that has been widely used in the production of high‐temperature alloys, (Mueller et al, 2000; Raffo, 1969; Wurster et al, 2010) as an additive for superconducting alloys (Ashkin et al, 1971; Singh et al, 2014) as a reforming catalyst in oil refineries, (Betizeau et al, 1976; Biloen et al, 1980; van Trimpont & Marin, 1986) for promoting syngas reaction catalysts, (Cook et al, 2014; Simonetti et al, 2007; Vada et al, 1995) and in nuclear medicine (Deutsch et al, 1986; Savio et al, 2001; Vucina & Han, 2003). Its abundance in the earth's crust is estimated to be <1 ppb and the annual production is several tons.…”
Section: Introductionmentioning
confidence: 99%