Lamellar Crystal-Dominated Surface of Polymer Film Achieved by Melt Stretching-Induced Free Surface Crystallization

Soft Matter ◽  
2021 ◽  
Author(s):  
Xiaohui Wang ◽  
Feifei Yan ◽  
Xue Bai ◽  
Hanchuan Li ◽  
Ming Yuan ◽  
...  

Lamellar crystal-dominated (LCD) surface holds great superiority and broad prospects for polymer surface engineering. The key to this is avoiding the formation of amorphous phase in the interlamellar region. Here...

Polymer ◽  
1993 ◽  
Vol 34 (5) ◽  
pp. 1089-1092 ◽  
Author(s):  
Shinichi Sakurai ◽  
Katsunori Tanaka ◽  
Shunji Nomura

2015 ◽  
Vol 7 (22) ◽  
pp. 11755-11764 ◽  
Author(s):  
Elena V. Agina ◽  
Alexey S. Sizov ◽  
Mikhail Yu. Yablokov ◽  
Oleg V. Borshchev ◽  
Alexander A. Bessonov ◽  
...  

1992 ◽  
Vol 25 (25) ◽  
pp. 7066-7068 ◽  
Author(s):  
Shinichi Sakurai ◽  
Katsunori Tanaka ◽  
Shunji Nomura
Keyword(s):  

1995 ◽  
Vol 413 ◽  
Author(s):  
A. Guiseppi-Elie ◽  
J. M. Tour ◽  
D. L. Allarat ◽  
N. F. Sheppard

ABSTRACTThin films of electroconductive poly[pyrrole-co-3−(1−pyrrolyl)propionic acid] were prepared by electropolymerization onto 3-aminopropyltrimethoxysilane modified and 3−(1−pyrrolyl)propionic acid derivatized interdigitated microsensor electrode (IME) arrays. The ω−(1−pyrrolyl) moiety on the surface of the device provides for specific adhesion of the polymer film to the device and the (N-pyrrolyl)propionic acid moiety on the polymer backbone provides for covalent attachment of bioactive molecules, such as biotin and urease, to the polymer surface. The immobilized, bioactive urease produces an ON/OFF conductimetric response traceable to analyte concentration.


Biomaterials ◽  
2014 ◽  
Vol 35 (26) ◽  
pp. 7488-7500 ◽  
Author(s):  
Mohammad-Ali Shahbazi ◽  
Patrick V. Almeida ◽  
Ermei M. Mäkilä ◽  
Martti H. Kaasalainen ◽  
Jarno J. Salonen ◽  
...  

2004 ◽  
Vol 843 ◽  
Author(s):  
Yong Yang ◽  
Ly James Lee

ABSTRACTPolymer-based Micro/Nano Electro Mechanical Systems (MEMS/NEMS) have attracted a great deal of interest from industries and academia. The common polymer processing methods involve either organic solvents or temperatures above the glass transition temperature (Tg), which is undesirable, particularly for biomedical applications. On the basis of different properties near polymer surfaces from those in the bulk, we introduce subcritical fluids (particularly carbon dioxide, CO2) into polymer surfaces to manipulate the polymer properties at the nanoscale so that we can achieve low temperature surface engineering. In this study, polymer surface dynamics under CO2 were addressed using atomic force microscopy (AFM) and neutron reflectivity (NR). Monodispersed nanoparticles were deposited onto the smooth polymer surface and then embedded into the surface by annealing the sample at the pre-specified temperatures and CO2 pressures. The embedding of nanoparticles in the proximity of the surface was measured using AFM, and thus the surface Tg profile could be determined. It was revealed that there is a rubbery layer of up to a hundred nanometers thick at the surface where the Tg is lower than that in the bulk and CO2 dramatically reduced the surface Tg. NR studies also show that CO2 can enhance chain mobility at the polymer surfaces below the polymer bulk Tg. These results indicated that even low concentrated CO2 greatly could enhance polymer chain mobility below the Tg of the CO2–plasticized polymers. The thickness of the rubbery layer can be controlled by tuning either temperatures, or CO2 pressures, or both, which makes it possible to engineer polymer surfaces at low temperatures. Guided by the CO2 enhanced polymer surface dynamics, we developed a novel CO2 bonding technique to succeed in low temperature bonding of polymers at the micro/nanoscales. This CO2 bonding technique has been applied to seal polymeric nanofluidic biochips and construct well-defined three-dimensional (3D) biodegradable polymeric tissue scaffolds.


2009 ◽  
Vol 419-420 ◽  
pp. 509-512
Author(s):  
Xi Qiu Fan

Based on viscoelastic fluid mechanics, this paper presents a simulation model of the flow behaviour of thin polymer film during nanoimprint lithography (NIL). The polymer is imprinted at a constant temperature of 180oC and at a constant imprint speed of 100nm/s by using a tool with a single convex feature of 100 nm in width and 500 nm in height. At the imprint beginning, only a very limited area adjacent to the tool top is affected by the imprint, but subjects to a sudden change of pressure. With the imprint process forward, the wave-like polymer front and the trumpet-shaped profile are predicted to travel out from the imprint patterns. When the tool base intimately contacts the polymer film, another sudden change of the pressure occurs in the area under the interface between the polymer surface and the tool base. These results are of significance to understand the flow behaviour of NIL.


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