2013
DOI: 10.1021/am404717j
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Realization of Metal–Insulator Transition and Oxidation in Silver Nanowire Percolating Networks by Terahertz Reflection Spectroscopy

Abstract: Metal nanowires (NWs) enable versatile applications in printed electronics and optoelectronics by serving as thin and flexible transparent electrodes. The performance of metal NWs as thin electrodes is highly correlated to the connectivity of NW meshes. The percolation threshold of metal NW films corresponds to the minimum density of NWs to form the transparent, yet conductive metal NW networks. Here, we determine the percolation threshold of silver NW (AgNW) networks by using morphological analysis and terahe… Show more

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Cited by 22 publications
(33 citation statements)
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References 29 publications
(41 reference statements)
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“…Due to the high effective mass m * = 23m 0 for the La 0.67 Ca 0.33 MnO 3 film, 23 we neglect the cyclotron resonance frequency = eB/m * . To understand the basic features of the complex conductivities, we employ the Drude–Smith model to analyze the experimental data, 28,29 where the dc conductivity = /m * , n is the carrier density, m * is the carrier effective mass, τ is the relaxation time, and c 1 denotes the fraction of the initial velocity of an electron after scattering events and varies between −1 and 0, which corresponds to localization and Drude formula, respectively. The complex conductivities and the fitted results at 105 K are shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Due to the high effective mass m * = 23m 0 for the La 0.67 Ca 0.33 MnO 3 film, 23 we neglect the cyclotron resonance frequency = eB/m * . To understand the basic features of the complex conductivities, we employ the Drude–Smith model to analyze the experimental data, 28,29 where the dc conductivity = /m * , n is the carrier density, m * is the carrier effective mass, τ is the relaxation time, and c 1 denotes the fraction of the initial velocity of an electron after scattering events and varies between −1 and 0, which corresponds to localization and Drude formula, respectively. The complex conductivities and the fitted results at 105 K are shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…[25][26][27][28][29][30] In this work the far-field transmittance spectra of our AgNW network was measured using a conventional THz time-domain spectrometer (THz-TDS), schematically represented in Figure 2a. [25][26][27][28][29][30] In this work the far-field transmittance spectra of our AgNW network was measured using a conventional THz time-domain spectrometer (THz-TDS), schematically represented in Figure 2a.…”
Section: Terahertz Far-field Spectroscopymentioning
confidence: 99%
“…One distinct point of the transverse dynamics for the individual NWs, apart from the longitudinal as well as from the bundled NWs dynamics, is that the excited carriers can be scattered off more easily from the NW surface [29]. While the high probability of carrier backscattering can be understood as the non-Drude conductivity spectrum [2], [30], [31], the electron and hole correlations within transverse region lead to multi-particle Auger scattering, by which the electron and hole are recombined nonradiatively. Consequently, the surface trap-mediated recombination is counterbalanced by this Auger scattering, revealing suppressed decay time constant in the individual SiNWs.…”
Section: Surface Trap Saturation and Auger Recombinationmentioning
confidence: 99%