1997
DOI: 10.1103/physrevb.56.10596
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Low-temperature resistance and its temperature dependence in nanostructured silver

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Cited by 47 publications
(29 citation statements)
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“…(1), shown in Table 1. The bulk mean free length of Ag is about 51 nm [14], which is much longer than the recrystallization grain size of the sintered Ag nanoparticles [ Fig. 3(c)].…”
Section: Resultsmentioning
confidence: 99%
“…(1), shown in Table 1. The bulk mean free length of Ag is about 51 nm [14], which is much longer than the recrystallization grain size of the sintered Ag nanoparticles [ Fig. 3(c)].…”
Section: Resultsmentioning
confidence: 99%
“…Since the wire dimensions are much larger than the mean free path of Ni then this enhancement in resistance value is owing to the effect of grainboundary scattering which is appeared to be predominant. It is needed to say that in nanocrystalline materials the resistivity temperature behavior ρ(T) is controlled by both phonon scattering, and interfacial scattering, and interfacial scattering enhances with decreasing temperature [5,6]. If the interfacial scattering becomes dominant, then the total resistance will possibly increases with decreasing temperature, showing nonmetallic behavior.…”
Section: Experimetal Detailsmentioning
confidence: 99%
“…[5] Thin films of silver have been deposited by many non-vacuum techniques including electrodeposition, [6] photochemical deposition, [7] electroless deposition, [8] and sol-gel. [9] Physical vapor deposition techniques include vacuum evaporation, [10] sputtering, [5,11,12] pulsed laser deposition, [13] electron beam evaporation, [14] and molecular beam epitaxy. [15] Among these various techniques, CVD has the advantage of potentially superior step-coverage, and is a single-step process which can easily be scaled up to deposit high purity films over large areas.…”
Section: Introductionmentioning
confidence: 99%