Numerical investigation of kinetic neuronic equations for one-dimensional neural system

1980 ◽  
Vol 36 (3) ◽  
pp. 125-130 ◽  
Author(s):  
F. Ventriglia
Keyword(s):  
Numerical Investigation ◽  
Neural System ◽  
One Dimensional

scholarly journals Numerical investigation of turbulent-jet primary breakup using one-dimensional turbulence

2017 ◽  
Vol 89 ◽  
pp. 241-254 ◽  
Author(s):  
A. Movaghar ◽  
M. Linne ◽  
M. Oevermann ◽  
F. Meiselbach ◽  
H. Schmidt ◽  
...  
Keyword(s):  
Numerical Investigation ◽  
Turbulent Jet ◽  
One Dimensional ◽  
Primary Breakup

Numerical investigation of the instability for one-dimensional Chapman–Jouguet detonations with chain-branching kinetics

2005 ◽  
Vol 9 (3) ◽  
pp. 385-401 ◽  
Author(s):  
H. D. Ng ◽  
M. I. Radulescu ◽  
A. J. Higgins ◽  
N. Nikiforakis ◽  
J. H. S. Lee
Keyword(s):  
Numerical Investigation ◽  
Chain Branching ◽  
One Dimensional

scholarly journals Numerical investigation of shock interaction with one-dimensional transverse array of particles in air

2016 ◽  
Vol 119 (10) ◽  
pp. 104901 ◽  
Author(s):  
Y. Mehta ◽  
T. L. Jackson ◽  
J. Zhang ◽  
S. Balachandar
Keyword(s):  
Numerical Investigation ◽  
Shock Interaction ◽  
One Dimensional

Numerical Investigation of Simultaneous Refractive index Sensor using 1D multichannel photonic crystal device

2020 ◽  
Author(s):  
A. Bouzidi ◽  
D. Bria ◽  
Hala J. El-Khozondar ◽  
D Vigneswaran ◽  
Shobhit K. Patel ◽  
...  
Keyword(s):  
Refractive Index ◽  
Titanium Dioxide ◽  
Photonic Crystal ◽  
Silicon Dioxide ◽  
Numerical Investigation ◽  
Refractive Index Sensor ◽  
Photonic Structure ◽  
One Dimensional ◽  
Numerical Studies ◽  
Three Samples

Abstract We present a multichannel sensor for the simultaneous monitoring of three different samples. established from a one-dimensional photonic crystal, this device is formed by an alternating layer of silicon dioxide (SiO2) and titanium dioxide (TiO2) with three defect layers containing the samples to be monitored. Numerical studies claim that three transmission peaks appear in the bandgap, these transmission peaks are caused by the three samples infiltrated in the defect layers. In real-time detection purposes, it is possible to exploit these transmission peaks. In addition, peak frequencies have the advantage of being susceptible to sample concentrations. With this photonic structure, a sensitivity of 800 nm per unit of refractive index (RIU) is reached.

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