Layer-by-layer deposition of Ti–4,4′-oxydianiline hybrid thin films

2011 ◽  
Vol 257 (15) ◽  
pp. 6435-6439 ◽  
Author(s):  
Anjali Sood ◽  
Pia Sundberg ◽  
Jari Malm ◽  
Maarit Karppinen
2015 ◽  
Vol 44 (44) ◽  
pp. 19194-19199 ◽  
Author(s):  
A. Tanskanen ◽  
M. Karppinen

Here we present novel layer-by-layer deposition processes for the fabrication of inorganic–organic hybrid thin films of the (–Fe–O–C6H4–O–)n type and also superlattices where N thicker iron oxide layer blocks alternate with monomolecular-thin organic layers.


2021 ◽  
Author(s):  
Kristina Ashurbekova ◽  
Karina Ashurbekova ◽  
Iva Saric ◽  
Evgeny Modin ◽  
Mladen Petravic ◽  
...  

We developed a thin film growth with a radical-initiated cross-linking of vinyl groups in a layer-by-layer manner via molecular layer deposition (MLD). The cross-linked film exhibited improved properties like 12% higher density and enhanced stability compared to the non-cross-linked film.


2009 ◽  
Author(s):  
Petronela Prepelita ◽  
R. Medianu ◽  
F. Garoi ◽  
A. Moldovan ◽  
A. M. Vlaicu

2014 ◽  
Vol 43 (9) ◽  
pp. 3492-3500 ◽  
Author(s):  
K. B. Klepper ◽  
O. Nilsen ◽  
S. Francis ◽  
H. Fjellvåg

We investigated the influence of the functionality of organic ligands on film properties in organic–inorganic hybrid thin films deposited by atomic layer deposition.


1992 ◽  
Vol 275 ◽  
Author(s):  
K. Yoshikawa ◽  
N. Sasaki

ABSTRACTUsing in-situ reflection high-energy electron diffraction (RHEED), we studied the growth of Bi-Sr-Ca-Cu-O (BSCCO) thin films prepared by reactive evaporation using layer-by-layer deposition. Bi2Sr2CaCu2Ox(2212) tends to be grown three-dimensionally if it is grown directly on (100) SrTiO3, in contrast to Bi2Sr2CuOx(2201) which is easily grown two-dimensionally on SrTiO3. Two-dimensional 2212 growth can be realized, if a buffer layer of 2201 is deposited on (100) SrTiO3 and growth interruption is utilized after SrO layer deposition. A buffer layer of only two 2201 unit cells improved the surface crystallinity of the substrate for the epitaxial growth of 2212. Growth interruption for two minutes after the 2nd SrO layer in the half unit cell is necessary to keep two-dimensional layered growth. The resulting Tc (zero) is 76 K and Jc (at 4.2 K) is 1.5 × 106 (A/cm2) with these epitaxial films.


Langmuir ◽  
2000 ◽  
Vol 16 (15) ◽  
pp. 6306-6311 ◽  
Author(s):  
Jun-ichi Anzai ◽  
Tomonori Hoshi ◽  
Nobuyuki Nakamura

1989 ◽  
Vol 169 ◽  
Author(s):  
Tomoji Kawai ◽  
Masaki Kanai ◽  
Hitoshi Tabata ◽  
Shichio Kawai

AbstractBy using 1ayer-by-1ayer successive deposition method with excimer laser ablation, the distance between CuO2 planes in the Bi2Sr2Ca1Cu2Oy superconductor has been controlled and super lattices with concentration modulation of Y and Ca have been formed. From the properties of these ‘Tailored films’, it is suggested that there is an interaction between CuO2 layers across Ca layer to affect the Tc value, but there is a very weak interaction across Bi2O2 blocking layers.


1998 ◽  
Vol 6 (2) ◽  
pp. 199-212
Author(s):  
Toshifumi Terui ◽  
Yusei Maruyama ◽  
Takeshi Arai ◽  
Shinro Mashiko

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