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Growth mechanism of photoreduced silver nanostructures on periodically proton exchanged lithium niobate : Time and concentration dependence

Carville, N. C. (författare)
Manzo, Michele (författare)
KTH,Kvantelektronik och -optik, QEO
Denning, D. (författare)
visa fler...
Gallo, Katia (författare)
KTH,Kvantelektronik och -optik, QEO
Rodriguez, B. J. (författare)
visa färre...
 (creator_code:org_t)
AIP Publishing, 2013
2013
Engelska.
Ingår i: Journal of Applied Physics. - : AIP Publishing. - 0021-8979 .- 1089-7550. ; 113:18, s. 187212-1-187212-7
  • Tidskriftsartikel (refereegranskat)
Abstract Ämnesord
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  • Photodeposition of metallic nanostructures onto ferroelectric surfaces, which have been chemically patterned using a proton exchange process, has recently been demonstrated. By varying the molar concentration of the AgNO 3 solution and the illumination time, one can determine the initial nucleation sites, control the rate of nucleation and the height of silver nanostructures formed, and study the mechanisms by which these processes occurs. The nanoparticles are found to deposit preferentially in the boundary between ferroelectric and proton exchanged regions, in an area proton exchanged via lateral diffusion under the masking layer used for chemical patterning, consistent with our previous results. Using a short illumination time (3 min), we are able to determine that the initial nucleation of the silver nanostructure, having a width of 0.17 ± 0.02 μm and a height of 1.61 ± 0.98 nm, occurs near the edge of the reactive ion etched area within this lateral diffusion region. Over longer illumination times (15 min), we find that the silver deposition has spread to a width of 1.29 ± 0.06 μm, extending across the entire lateral diffusion region. We report that at a high molar concentration of AgNO3 (10-2 M), the amount of silver deposition for 5 min UV illumination is greater (2.88 ± 0.58 nm) compared to that at low (10-4 M) concentrations (0.78 ± 0.35 nm), however, this is not the case for longer time periods. With increasing illumination time (15 min), experiments at 10-4 M had greater overall deposition, 6.90 ± 1.52 nm, compared to 4.50 ± 0.76 nm at 10 -2 M. For longer exposure times (30 min) at 10-2 M, the nanostructure height is 4.72 ± 0.59 nm, suggesting a saturation in the nanostructure height. The results are discussed in terms of the electric double layer that forms at the crystal surface. There is an order of magnitude difference between the Debye lengths for 10-2 and 10-4 M solutions, i.e., 3.04 vs. 30.40 nm, which suggests the Debye length plays a role in the availability of Ag ions at the surface.

Ämnesord

NATURVETENSKAP  -- Fysik (hsv//swe)
NATURAL SCIENCES  -- Physical Sciences (hsv//eng)

Nyckelord

Chemical patterning
Concentration dependence
Electric double layer
Ferroelectric surfaces
Metallic nanostructure
Molar concentration
Proton exchange process
Silver nanostructures
Deposition
Diffusion
Ferroelectricity
Nucleation
Nanostructures

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Av författaren/redakt...
Carville, N. C.
Manzo, Michele
Denning, D.
Gallo, Katia
Rodriguez, B. J.
Om ämnet
NATURVETENSKAP
NATURVETENSKAP
och Fysik
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Journal of Appli ...
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Kungliga Tekniska Högskolan

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