photonic stop band
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2021 ◽  
Vol 117 ◽  
pp. 111146
Author(s):  
Bhargavi Veeraghattam ◽  
Prasanta Kumar Guha ◽  
B.N. Shivakiran Bhaktha

2021 ◽  
Vol 23 (36) ◽  
pp. 20275-20281
Author(s):  
Matin Ashurov ◽  
Bakhodur Abdusatorov ◽  
Alexander Baranchikov ◽  
Sergey Klimonsky

The detection limit of methylene blue of about 10−7 M was achieved by measuring Raman scattering of light at a laser wavelength that coincides with the photonic stop band of a composite substrate consisting of inverse opal with gold nanoparticles.


2020 ◽  
Vol 22 (17) ◽  
pp. 9630-9636
Author(s):  
Matin Ashurov ◽  
Alexander Baranchikov ◽  
Sergey Klimonsky

Inverse opal films impregnated with a methylene blue dye were prepared by a template route. Photonic stop band governs amplitude of spontaneous Raman scattering peaks for metal-free photonic crystals, enhancement factor being over 50.


2019 ◽  
Vol 18 (03n04) ◽  
pp. 1940044 ◽  
Author(s):  
Yu. D. Karnilava ◽  
P. A. Kholov ◽  
N. V. Gaponenko ◽  
T. F. Raichenok ◽  
S. A. Tikhomirov ◽  
...  

With the use of sol–gel method BaTiO3–SiO2 multilayer structures were fabricated on glass or fused silica substrates employing dipping or spinning procedure. The photonic stop band was observed in the reflection and transmission spectra of the multilayer structure annealed at [Formula: see text]C. It is redshifted with an increase of the thicknesses of BaTiO3 and SiO2 layers. For structures comprising Eu-doped BaTiO3 layers of different thicknesses photoluminescence with the main band at 614[Formula: see text]nm was detected. It is characterized with the double-exponential decay with the lifetimes of about 0.5[Formula: see text]ms and 1.1[Formula: see text]ms which do not depend significantly on the photonic stop band position.


2018 ◽  
Vol 8 ◽  
pp. 184798041878840
Author(s):  
Valentina Robbiano ◽  
Salvatore Surdo ◽  
Alessandro Minotto ◽  
Giancarlo Canazza ◽  
G Mattia Lazzerini ◽  
...  

Loading of one-dimensional (1-D) porous silicon photonic crystals (PS-PhCs), known as rugate filters, with luminescent materials is generally limited by the potential for (undesired) “pore clogging,” in relation to the size of the nanoparticles (e.g. quantum dots) or molecular species, and so far mainly restricted to small molecular weight materials or small nanocrystals, or in situ polymerized dyes. Here we report the infiltration 1-D PS-PhCs with a green-emitting commercial luminescent polymer (F8BT, poly[(9,9-di-n-octylfluorenyl-2,7-diyl)-alt-(benzo[2,1,3]thiadiazol-4,8-diyl)]), with a molecular weight of approximately 46 kDa across their whole depth (approximately 7.5 μm), thereby showing that pore clogging is not a concern for these structures. We also characterize the modification of the photoluminescence (PL) and decay rates, and investigate the detailed inner morphology of the filters with the help of (scanning) transmission electron microscopy. We observe both suppression (in the stop-band) and enhancement (at the high-energy band-edge) of the PL. We also find that the photonic stop-band is red-shifted after polymer infiltration, due to the increased effective refractive index of the polymer-infiltrated nanostructured system. The presence of just one unbroadened peak in the reflectance spectra after infiltration confirms that infiltration extends for the whole depth of the rugate filters.


2017 ◽  
Vol 110 (25) ◽  
pp. 251104 ◽  
Author(s):  
Anirban Sarkar ◽  
N. N. Subhashree Ojha ◽  
B. N. Shivakiran Bhaktha

2017 ◽  
Vol 118 (7) ◽  
Author(s):  
L. G. Helt ◽  
Agata M. Brańczyk ◽  
Marco Liscidini ◽  
M. J. Steel

2013 ◽  
Vol 25 (22) ◽  
pp. 3106-3110 ◽  
Author(s):  
You Feng Yue ◽  
M. Anamul Haque ◽  
Takayuki Kurokawa ◽  
Tasuku Nakajima ◽  
Jian Ping Gong

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