Analysis of Biomolecular Interaction Process Based on SPR Imaging Method in Microfluidic Chips

Plasmonics ◽  
2021 ◽  
Author(s):  
Honggang Wang ◽  
Huixiang Wang ◽  
Zhen Tian ◽  
Hao Zhang ◽  
Yafeng Huang ◽  
...  
Author(s):  
Marie-Bernadette Villiers ◽  
Sandra Cortès ◽  
Carine Brakha ◽  
Patrice Marche ◽  
André Roget ◽  
...  

2020 ◽  
Vol 8 (39) ◽  
pp. 13563-13573
Author(s):  
Xueyi Luo ◽  
Shijie Deng ◽  
Peng Wang

A surface plasmon resonance (SPR) imaging method for monitoring the electric double-layer (EDL) change dynamics in real-time and map the lateral EDL distribution on heterogeneous electrode/electrolyte interface.


Author(s):  
T. Y. Tan ◽  
W. K. Tice

In studying ion implanted semiconductors and fast neutron irradiated metals, the need for characterizing small dislocation loops having diameters of a few hundred angstrom units usually arises. The weak beam imaging method is a powerful technique for analyzing these loops. Because of the large reduction in stacking fault (SF) fringe spacing at large sg, this method allows for a rapid determination of whether the loop is faulted, and, hence, whether it is a perfect or a Frank partial loop. This method was first used by Bicknell to image small faulted loops in boron implanted silicon. He explained the fringe spacing by kinematical theory, i.e., ≃l/(Sg) in the fault fringe in depth oscillation. The fault image contrast formation mechanism is, however, really more complicated.


Author(s):  
Akira Tonomura

Electron holography is a two-step imaging method. However, the ultimate performance of holographic imaging is mainly determined by the brightness of the electron beam used in the hologram-formation process. In our 350kV holography electron microscope (see Fig. 1), the decrease in the inherently high brightness of field-emitted electrons is minimized by superposing a magnetic lens in the gun, for a resulting value of 2 × 109 A/cm2 sr. This high brightness has lead to the following distinguished features. The minimum spacing (d) of carrier fringes is d = 0.09 Å, thus allowing a reconstructed image with a resolution, at least in principle, as high as 3d=0.3 Å. The precision in phase measurement can be as high as 2π/100, since the position of fringes can be known precisely from a high-contrast hologram formed under highly collimated illumination. Dynamic observation becomes possible because the current density is high.


1950 ◽  
Vol 14 (3) ◽  
pp. 235-235
Author(s):  
No authorship indicated

2011 ◽  
Vol 59 (S 01) ◽  
Author(s):  
S Ihlenburg ◽  
A Rüffer ◽  
T Radkow ◽  
A Purbojo ◽  
M Glöckler ◽  
...  

2008 ◽  
Vol 39 (01) ◽  
Author(s):  
AJ Fallgatter ◽  
AC Ehlis ◽  
MM Richter ◽  
M Schecklmann ◽  
MM Plichta

2013 ◽  
Vol E96.B (7) ◽  
pp. 2014-2023 ◽  
Author(s):  
Ryo YAMAGUCHI ◽  
Shouhei KIDERA ◽  
Tetsuo KIRIMOTO

Sign in / Sign up

Export Citation Format

Share Document