Design of a silicon-based ultracompact polarization splitter (PS) with high extinction ratio (ER) is proposed for the midinfrared-operating wavelength of 4.47 μm. It is based on a directional coupler (DC) that consists of a horizontal slot waveguide (WG) and a strip WG with Si as the core material and CaF2 as the slot and substrate material. By choosing appropriate structural parameters, we have designed the DC-PS such that only the TM polarization satisfies the phase-matching condition for coupling at the targeted wavelength of 4.47 μm; achieved ERs are ∼41.6 dB and ∼37.1 dB for the cross-coupled and the throughput ports, respectively. Corresponding estimated insertion losses (ILs) are ∼0.25 dB and ∼0.07 dB in a device length of just ∼6.6 μm. Over a broad bandwidth of 200 nm (4.37 to 4.57 μm) in the mid-IR, our designed PS exhibited ER of >37 dB (with IL of <0.5 dB) for the cross-coupled port and an ER of >17 dB (with IL of <0.1 dB) for the throughput port. Numerical estimations revealed excellent tolerance to the potential fabrication errors.
We have numerically demonstrated refractive index sensing using terahertz metamaterials comprised of single split gap resonators. Sensing capabilities of odd and even order resonance modes are precisely investigated. In this scheme the top surface of metamaterials array is covered with a thin layer of polyimide whose refractive could be changed manually. The sensitivity and corresponding figure of merit (FoM) of several lowest order modes are examined with respect to the different thicknesses of the coated polyimide film. We have investigated the electric field distributions at different resonances for the MMs. Although we have mainly focused on refractive index sensing but this study could be extremely useful for the development of metamaterials based sensing devices, bio-sensors etc.
Presence of photonic band-gap (PBG) in an all-solid microstructured optical fiber (MOF), made of two fabrication
compatible chalcogenide (Ch) glasses is theoretically investigated for potential application in the functional mid-infrared
(IR) wavelength range. Cross-section of the MOF is formed by assuming periodically arranged wavelength scale circular
air holes in a hexagonal pattern embedded in a uniform matrix. One type of Ch-glass is considered as the background
material whereas another type of Ch-glass is assumed to fill the air holes. The relative index contrast between these two
Ch-glasses is ~ 24%, for which PBG appears only for a suitable range of non-zero longitudinal wave vector. We have
studied the scalability of this PBG by varying the lattice parameter of MOF and optimized the cross-section to attain the
PBG at ~ 2 μm wavelength. Then by utilizing the thermo-optic properties of the glasses, the effect of external
temperature (T) on the PBG is studied, and finally we have proposed a T-tunable wavelength filter/sensor at mid-IR
wavelength with tuning sensitivity as high as ~ 140 pm/°C.
Fiber directional couplers made of highly asymmetric twin-cores (ATC), one of which is doped with erbium, are
designed to achieve an inherently gain flattened erbium doped fiber amplifier (EDFA). The refractive index profiles of
the fibers as well as the spacing between the two cores were carefully designed to achieve a targeted gain with low gain
excursions across the C-band. One of the designs yielded a theoretical median gain ~ 38 dB with an excursion within ±1
dB. In order to suite fabrication of such an inherently gain flattened EDFA by the MCVD fiber preform fabrication
process, the design had to be modified and a more modest target of about 20 dB was set with excursion below ± 1.5 dB
for metro-centric applications. It involved preparation of two independent preforms, which required selective polishing
of the cladding from one side by a certain amount to meet the required nominal separation between the two cores set at
the design stage of the fiber. Several intricate operations were required to implement the fiber drawing step from the two
assembled preforms. Preliminary characterization of the fabricated fiber shows filtering of ASE peak through selective
wavelength coupling from Er-doped core to un-doped core.
We present a high sensitive temperature sensor based on a side-polished fiber (SPF) coupled to a tapered multimode
overlay waveguide (MMOW). We have theoretically shown that the longitudinal tapering of the MMOW can be used to
tune the desired wavelength range in the spectrum without any loss in the sensitivity.
We investigate the inherent gain flattening characteristics of an EDFA based on a highly asymmetric dual-core photonic
crystal fiber for operation in the C-band. The gain flattening was achieved by exploiting the strong optical power
coupling between the two cores like that in a directional coupler at the phase matching wavelength (λ Ρ), which is
designed to be around 1533 nm. The inner core is partially doped with erbium. The fiber refractive index profile
parameters were so tailored such that a large fraction of the composite guided power flips from the un-doped outer core
to the inner erbium-doped core at wavelengths greater than λ Ρ. Thus the guided power at relatively longer wavelengths
gets amplified more as compared to that at shorter wavelengths in the C-band. This phenomenon resulted in an effective
flattening of the gain spectrum. Optimization of the design has led to an estimated median gain of ~ 21.2 dB with gain
excursion within ± 1.25 dB within the C-band (1532-1562 nm). Results of this work should be of importance for
realizing relatively inexpensive (due to cost saving on gain flattening filter head) and efficient EDFAs suitable for
potential deployment in transparent wide area and metro networks.
We propose a method for sensing the turbidity of a solution by inserting a fiber-optic probe in conjunction with a mirror.
The probe consists of seven fibers, which illuminate as well as collect the light scattered from the sample after reflection
from the mirror, in order to estimate the turbidity of the sample solution. We have estimated turbidity in terms of total
interaction coefficient, a parameter that contains strong signature of the turbidity of a liquid. A light-scattering model
based on Monte Carlo simulations is employed to simulate the power collected by the probe, which match reasonably
well with the experimental results. The method is simple, and should be useful for detecting suspended impurities in a
liquid even in small quantities.
A high sensitive temperature sensor based on evanescent field coupling between a side-polished fiber half-coupler
(SPFHC) and a thermo-optic multimode overlay waveguide (MMOW) is designed and demonstrated. Such a structure
essentially functions as an asymmetric directional coupler with a band-stop characteristic attributable to the wavelengthdependent
resonant coupling between the mode of the SPFHC and one or more modes of the MMOW. A slight change in
temperature leads to a significant shift in the phase resonance-coupling wavelength ( λr ) between the MMOW and
SPFHC λr, which is easily measurable. The wavelength sensitivity of the device is measured to be ~ 5.3 nm/°C within
the measurement range of 26-70°C; this sensitivity is more than 5 times higher compared to earlier reported temperature
sensors of this kind. The SPFHC was fabricated by selective polishing of the cladding from one side of a bent
telecommunication standard single-mode fiber and the MMOW was formed on top of the SPFHC through spin coating.
A semi- numerical rigorous normal mode analysis was employed at the design stage by including the curvature effect of
the fiber lay in the half-coupler block and the resultant
z-dependent evanescent coupling mechanism. An excellent
agreement between theoretical and experimental results is found.
An all-fiber interferometric experimental technique to determine the mode effective index neff of a single-mode fiber is proposed. The method involves setting up an unbalanced Mach-Zehnder interferometer (MZI) with the test fiber. By inducing a small change in the differential path length between the two arms of the MZI, a proportional change in the periodicity of its transmission spectrum could be introduced. A precise measurement of this change in periodicity has been used to accurately determine the value of neff of the test fiber.
We present an analysis of fused fiber couplers by simultaneously considering the coupling of guided modes through the overlap of the evanescent fields in the weakly interacting 'taper transition' region as well as the beating of cladding modes in the strongly interaction 'taper waist' region. We have incorporated geometrical parameters to account for the 'degree of fusion' and the 'shape of taper', thus representing a realistic coupler structure. The results of our model are in very good agreement with the measured characteristics of coupler components fabricated in our laboratory.
A novel frequency domain simulator is developed for simulation of large size WDM system considering the spectrum evolution of each of the WDM channel impaired by the simultaneous effect of group velocity dispersion, self-phase modulator and cross-phase modulation. The frequency domain approach has been made possible by linearly the relationship p between Fourier transform of input and output power profile and phase over small step size.
We report in-house development of a real time monitoring system with programmable fabrication parameters for fabricating fused-fiber coupler based branching components. A number of branching components of varied specifications and with fibers of different make have been fabricated; these exhibited low excess loss and other features akin to commercially available couplers. Fabricated WDM couplers for operation at 1310/1550 nm exhibited high degree of isolation, large isolation bandwidth and reasonably low excess loss. Characteristics of the fabricated couplers have been investigated for optimizing design and fabrication parameters with regard to channel isolation and excess loss in the device. An equivalent planar waveguide (EPG) model has also been used to model these couplers and to correlate with the experimental findings.
Fiber components based on evanescent coupling of a side-polished single-mode fiber to a highly multimode active/passive overlay k waveguide form an important class of a host of in-line fiber components. We report a normal mode analysis to accurately model such fiber components. Our model yields complete transfer function of all such components/devices. The method is extended to analyze certain very recently proposed semiconductor clad dielectric waveguides which find applications in integrated optics
Low-loss high-silica fibers were first reported in 1970 and since then these glass fibers have proven to be the most viable transmission media for lightwave communication. Even though the first low loss fiber was a single-mode fiber, initial systems revolved around multimode fibers from the point of view of practical reasons like easier fiber to fiber splicing and coupling from off-the-shelf available LEDs. Since early 1980s, single-mode fibers became the preferred media for optical transmission and single-mode fibers overtook the multimode fibers for lightwave communication. Networks which operate with single-mode fibers at the 1.31 /mm low-loss wavelength window are now taken for granted. Operations with advanced fiber designs at the silica fiber’s lowest loss window of 1.55 /mm are now gearing to take over the long-haul routes; these are contemplated to be based on erbium doped fiber amplifiers (EDFA) and dispersion shifted fibers. An alternative and promising scheme for this wavelength window involving use of already laid fibers optimized for 1.31 /an requires insertion of a dispersion compensating fiber(DCF) as an additional component in the link. In the immediate future, lightwave systems would operate with EDFA at the OC-48 level, which amounts to a bit rate of — 2.5 Gb/s and are compatible with SDH (STM-16) networks. For WDM transmission with EDFAs, one would require a variety of in-line fiber components like wavelength selective couplers, and bandpass/bandstop filters to add/drop channels. Until recently, optical fibers were considered to be optically linear. However, with the introduction of EDFAs, which provide large and broadband (* 30-35 nm) optical gains, a large number of WDM information channels can be transmitted and simultaneously provided gains across this broad gain spectrum of EDFAs. Furthermore, amplifier spacings could be much longer than the present day regenerator spacings. These two fall outs of EDFA namely, large optical power density and long interaction lengths have elevated optical fiber nonlinearities to an important design issue in lightwave systems. In this presentation we would aim to trace the evolutionary trends in lightwave communications seen along the above lines since the reporting of the first low-loss fibers a quarter century ago. INTRODUCTION
A novel scheme for simultaneous compensation of dispersion and loss is proposed. This should be realizable by doping an optical fiber having a high negative dispersion coefficient at 1.55 /mm with erbium ions. Numerical calculations are presented for a typical design example. Such an erbium doped dispersion compensating fiber (ED-DCF) should be a promising alternative as a more compact unit as compared to the spliced combination of an EDFA and DCF as two distinct components.
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