2010
DOI: 10.2478/s11772-010-0046-3
|View full text |Cite
|
Sign up to set email alerts
|

Self-assembly: mastering photonic processes at nanoscale

Abstract: Supramolecular ordering happens as an important parameter for the control of light emission processes. In this review paper, we discuss several examples of application of self-assembly to the realization of nano-structures designed in view of mastering specific photonic processes. This comprises the formation of highly localized plasmon modes in self-organized 2D assemblies of metal nanoparticles, the immobilization of dyes inside highly homogeneous 2D alveolar self-assembled molecular matrices and molecular 3… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
2
0

Year Published

2011
2011
2017
2017

Publication Types

Select...
4

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 60 publications
0
2
0
Order By: Relevance
“…The nucleation into a self-assembled structure takes finite time after the critical saturation ratio is reached; that is, there is a delay before nucleation takes place. The delay time for nucleation (τ d ) is given by the following equation: 49 2 DNc e S(ln S) 3 (9) where v 0 is the molecular volume of dye, σ is the surface energy of the self-assembled material, γ* is the accommodation coefficient in solution, which is ∼1, k is the Boltzmann constant, T is the temperature, D is the monomer diffusion coefficient in the solvent, solvent, N is Avogadro number, c e is the equilibrium solubility, and S is the saturation ratio. At a critical saturation ratio (S*), the time delay for nucleation will be constant irrespective of the initial concentration.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The nucleation into a self-assembled structure takes finite time after the critical saturation ratio is reached; that is, there is a delay before nucleation takes place. The delay time for nucleation (τ d ) is given by the following equation: 49 2 DNc e S(ln S) 3 (9) where v 0 is the molecular volume of dye, σ is the surface energy of the self-assembled material, γ* is the accommodation coefficient in solution, which is ∼1, k is the Boltzmann constant, T is the temperature, D is the monomer diffusion coefficient in the solvent, solvent, N is Avogadro number, c e is the equilibrium solubility, and S is the saturation ratio. At a critical saturation ratio (S*), the time delay for nucleation will be constant irrespective of the initial concentration.…”
Section: Resultsmentioning
confidence: 99%
“…Self-assembled materials are gaining in importance due to their special properties and applications in different areas such as solar cells, , photonics, , organic semiconductors, , recording media, and development of biomaterials. , Molecular self-assembly is used to synthesize new materials such as liquid crystals and semicrystalline and phase-separated polymers . Molecular self-assembly is defined as spontaneous assembly under equilibrium conditions to form stable aggregates; the process can entail formation of covalent or noncovalent bonds .…”
mentioning
confidence: 99%