Abstract: The principle of all-silicon Raman lasers for an
output wavelength of 1.3 μm is presented, which employs
quasi-phase-matched structures and resonators to enhance the output
power. 1.3-μm laser beams for GE-PONs in FTTH systems generated
from a silicon device are very important because such a silicon device
can be monolithically integrated with the silicon planar lightwave
circuits (Si PLCs) used in the GE-PONs. This reduces the device
fabrication processes and time and also optical losses at the junctions
between optical waveguides of the Si PLCs and Si laser devices
when compared with 1.3-μm III-V semiconductor lasers set on the
Si PLCs employed at present. We show that the quasi-phase-matched
Si Raman laser with resonators can produce about 174 times larger
laser power at 1.3 μm (at maximum) than that without resonators
for a Si waveguide of Raman gain 20 cm/GW and optical loss 1.2
dB/cm, pumped at power 10 mW, where the length of the waveguide
is 3 mm and its cross-section is (1.5 μm)2.
Abstract: This paper presents an investigation of the fabrication of the optical devices in terms of their characteristics based on the use of the electromagnetic waves. Planar waveguides are used to examine the field modes (bound modes) and the parameters required for this structure. The modifications are conducted on surface plasmons based waveguides. Simple symmetric dielectric slab structure is used and analyzed in terms of transverse electric mode (TE-Mode) and transverse magnetic mode (TM-Mode. The paper presents mathematical and numerical solutions for solving simple symmetric plasmons and provides simulations of surface plasmons for field confinement. Asymmetric TM-mode calculations for dielectric surface plasmons are also provided.
Abstract: Refractive index control of benzocyclobutene (BCB 4024-40) is achieved by facilitating different conditions during the thermal curing of BCB film. Refractive index (RI) change of 1.49% is obtained with curing of BCB film using an oven, while the RI change is 0.1% when the BCB is cured using a hotplate. The two different curing methods exhibit a temperature dependent refractive index change of the BCB photosensitive polymer. By carefully controlling the curing conditions, multiple layers of BCB with different RI can be fabricated, which can then be applied in the fabrication of optical waveguides.