TY - JOUR
T1 - Terahertz polarization controller based on electronic dispersion control of 2D plasmons
AU - Nishimura, Takuya
AU - Otsuji, Taiichi
N1 - Funding Information:
The authors thank Profs. K. Narahara, E. Sano, and V. Ryzhii for their valuable discussion. This work was financially supported in part by the SCOPE program from the MIC, Japan and the Grant in Aid for Scientific Research (S) from the JSPS, Japan.
PY - 2007/9
Y1 - 2007/9
N2 - We numerically investigated the possibility of terahertz polarization controller based on electronic dispersion control of two dimensional (2D) plasmon gratings in semiconductor heterostructure material systems. Taking account of the Mikhailov's dispersive plasmonic conductivity model, the electromagnetic field emission properties of the gated 2D plasmon gratings were numerically analyzed with respect to the density (n) of electrons by using in-house Maxwell's FDTD (finite difference time domain method) simulator. When n is low under a constant drift-velocity condition, the fundamental plasmon mode is excited, being coupled with the radiative zeroth mode of transverse electric (TE) waves. When n exceeds a threshold level, the second harmonic mode of plasmon is predominantly excited, being coupled with the non-radiative first mode of TE waves. We numerically demonstrated that if a grating mesh of 2D plasmons is formed where two independent 2D plasmon gratings are combined orthogonally, the structure can act as a polarization controller by electronically controlling the two axial plasmonic dispersions.
AB - We numerically investigated the possibility of terahertz polarization controller based on electronic dispersion control of two dimensional (2D) plasmon gratings in semiconductor heterostructure material systems. Taking account of the Mikhailov's dispersive plasmonic conductivity model, the electromagnetic field emission properties of the gated 2D plasmon gratings were numerically analyzed with respect to the density (n) of electrons by using in-house Maxwell's FDTD (finite difference time domain method) simulator. When n is low under a constant drift-velocity condition, the fundamental plasmon mode is excited, being coupled with the radiative zeroth mode of transverse electric (TE) waves. When n exceeds a threshold level, the second harmonic mode of plasmon is predominantly excited, being coupled with the non-radiative first mode of TE waves. We numerically demonstrated that if a grating mesh of 2D plasmons is formed where two independent 2D plasmon gratings are combined orthogonally, the structure can act as a polarization controller by electronically controlling the two axial plasmonic dispersions.
KW - 2D plasmon gratings
KW - Dispersion control
KW - Plasmon resonance
UR - http://www.scopus.com/inward/record.url?scp=41149150368&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=41149150368&partnerID=8YFLogxK
U2 - 10.1142/S0129156407004734
DO - 10.1142/S0129156407004734
M3 - Article
AN - SCOPUS:41149150368
VL - 17
SP - 547
EP - 555
JO - International Journal of High Speed Electronics and Systems
JF - International Journal of High Speed Electronics and Systems
SN - 0129-1564
IS - 3
ER -