A double series configuration of a microresonator is proposed to measure the amount of corrosion on iron metal. A numerical computation has been performed for analyzing the sensing operation in which the metal is attached to the waveguide as a top cladding material. The transparency peak profile and transfer function of the output transmission spectrum is obtained using a signal flow graph method and Mason’s rule. The output spectrum of the microresonator shows that the linear free spectral range (FSR) changes as the iron begins to oxidize, which affects the cladding index of the sensing system. The FSR changes with respect to the amount of corrosion present in iron metal. In addition, the microresonator is able to distinguish two different types of corrosion, which are hematite and magnetite. The sensitivities of the practical application design are obtained as 22.62 nm/RIU for magnetite and 7.17 nm/RIU for hematite detection. The FSR analysis is an alternative approach in all-optical sensing to wavelength shift. It is promising for applications in additional high-sensitivity all-optical corrosion sensors.
We propose a novel design of optical buffer to generate slow light based on delay time. In the framework of the nonlinear waveguide, we investigate propagation of solitons through microring resonators. Dynamical control over slow-light solitons is realized via controlling fields generated by bright soliton and Gaussian pulse. The nonlinear dependence of the velocity of the signal on the controlling field is analytically described. The buffering effect is achieved by slowing the optical signal using an external control light source to vary the dispersion characteristic of the medium via microring resonators. A graphical approach with a signal flow graph method is used to derive the optical transfer functions in z-domain of filters. The characteristics of the optical buffer devices including the transmittance and time delay of the through and drop port are simulated. Simulated results show the criteria of achieving slow light in semiconductor microring resonators. Finally, output signal shows the delay time rate by propagation through the semiconductor microring resonators.
In this study a new design of terahertz frequency carrier generation for radio frequency identification (RFID) application is proposed. The dense wavelength-division multiplexing can be generated and obtained by using a Gaussian or soliton pulse propagating within a modified add-drop filter known as a PANDA ring resonator. The broad bandwidth of terahertz signals can be obtained and are available for useful applications, in which the use of the generated terahertz pulses for RFID application, for instance Ad-Hoc network, uses RFID. Results obtained have shown that the increase in channel capacity can be obtained and useful for the large demand of RFID applications.
Fabrication of single-mode fiber coupler has widely expands. However, directional fiber coupler
geometry always affects the power propagation either two or three ports. This paper describes
power launching by NX3 single mode fiber, examined using a matrix transfer for linear and
triangle order, calculated from the eigenvalue and the eigenvector. This eigenvalue is referred to
the coupling coefficient, where it can be expressed as an effective power transmitted to another
fiber. The ratio of coupling coefficient between adjacent axial fibers varies, which can be
achieved by adjusting separation of fiber and refractive index of core and cladding. A calculation
has been shown in 3D that both power transmission and phase are affected by not only the
geometry order, but also the variation of coupling coefficient, assuming the propagation
constants, cross section, and separation of coupling length fiber axis are held constant. This
calculation can be applied for any sources of wavelength and junction.
This paper describes a new model for the breakdown voltage of SiO2 fiber coupler using the Pockel effect and empirical
equation. The model is evaluated by using the coupling coefficient and the changes in the refractive index. We found that
the breakdown voltage is in the order of 102 volt correspond to coupling coefficient by the order of mm-1. Increasing the
value of coupling coefficient between the electrodes leads to a reduction in the breakdown voltage.
We propose a novel system of broadband source generation using a common soliton pulse (i.e., with center wavelength at 1.55 µm) propagating within a nonlinear micro-ring resonator system. The system consists of a micro-ring resonator system incorporating an add/drop filter, whereby the large-bandwidth signals can be generated, stored, and regenerated within the system. By using the appropriate parameters relating to the practical device such as micro-ring radii, coupling coefficients, and linear and nonlinear refractive index, we found that the obtained multisoliton pulses have shown the potential of application for dense wavelength-division multiplexing (DWDM), whereby the different center wavelengths of the soliton bands can be obtained via the add/drop filter, which can be used to increase the communication channel capacity in the communication network. The best free spectra range (FSR) and FWHM of the results obtained are 14 nm and 100 pm, respectively, which allows an increase in channel capacity of at least 10 times in only one center wavelength.
In this paper we present theoretical and experimental analysis on Nd:YAG laser microwelding for pigtailing laser diode
transmitter through two ball lenses that are employed for effectively matching the elliptical mode field of the laser diode
with the circular on of the single mode fiber. The fiber attachment and the fixing of various coupling components have
been performed in what is so called active alignment process. The system continues measuring the coupled power during
the processes of alignment and attachment of various coupling components as well as the working distance and
misalignment tolerances optimizations. Results of theoretical modeling of laser weld penetration depth agree with the
experimentally measured results in the low laser pulse energy range. Moreover the laser pulse parameters such as,
duration, energy, number of pulse shoots as well as the focusing position over the workpiece and angle of laser pulse
incidence are found to have very significant effects on the weld yields and greatly affect the laser weld depth to width
ratio. Optimization of all the mentioned parameters found to be necessary for achieving strong laser microwelds with
more penetration and less width in the attachments of the sensitive optical components inside the packaged photonic devices modules.
Coupled 1X2 Single Mode Fiber (SMF-28e"R") has been successfully fabricated using a slightly unstable torch flame at a
temperature range of 800°C to 1350°C injecting hydrogen gas flowing at pressure of 1 bar. The coupling ratio and
coupling coefficient can be examined from 1% until 75%. In this paper, we compare the experimental results by using a
simple kinetic model of coupling coefficient where internal and external parametric functions are considered. This
equation is time independent and is then integrated over the direction of the coupling ratio range for various separation
fibers axis between two cores. The result shows that the separation between the cores significantly affects coupling
coefficient exhibiting exponential behavior. In the experiment the coupling coefficient gradient is significantly changed
towards the coupling ratio but in modeling it has a function of separation fiber axis and no power imposed. These
phenomena will determine the effects of power losses at coupling region where fabrications of coupled fibers are
demonstrated.
In this paper we present analysis on three different coupling systems, i.e., butt, single ball lens, and two ball lenses
between the tips of two coupled single mode fiber in semiconductor optical amplifier (SOA) module. The coupling
components inside the module can be aligned in an active alignment process and attached by means of dual beam from
an Nd: YAG laser welding system. The tips of the coupled fiber are ferruled inside metallic tubes to enable the
attachment to the substrates through saddle-shaped welding clips. Investigations of the variations of coupling efficiency
with the with working distance for the three schemes showed that two ball lenses is more efficient with coupling
efficiency of 75% followed by single ball lens at 55% and butt coupling mode at 20% maximum. In addition dual ball
lens configuration have shown to have better longitudinal tolerant even with an elliptical beam profile from the source
fiber. This is however not the case in single ball lens and butt coupling scheme. We also observe however the optimum
separation between the two lenses at in the range between 0.35 mm - 0.45 mm. This is to ensure the coupling efficiency
is the highest possible within the acceptable tolerant misalignments.
Fiber couplers are widely used in telecommunication and industry as a passive splitting power device. The effective
power coupling and transmitting from one fiber to another is mainly determined by both coupling length and coupling
coefficient. Coupling length can be calculated directly but for coupling coefficient it depends upon the refractive index
and separation fiber axis. After fusion processes of two SMF-28e(R) couplers, the refractive index is unknown due to
change in the radius of fiber (rcladd<40μm and rcore<1.5μm). Coupling coefficient range is obtained from a distribution of
coupling ratio and compared with the empirical formula which also enables to calculate refractive index. In this
experiment, coupling coefficient in the range of 0.6-0.9/mm is calculated as a function of separation fiber axis and
refractive index of core and cladding. The result shows a good correlation between experimental results and theoretical
calculation.
This paper presents some analysis for the matching between the elliptical mode field of 1550nm high power laser diode with
the circular mode field of the single mode fiber in order to obtain high coupling efficiency with relaxed misalignment
tolerances. Three coupling schemes namely Butt, single ball lens and double ball lenses coupling schemes have been
employed in pigtailing the butterfly laser diode module using laser welding technique with dual beams from Nd:YAG laser
welding system for the attachment of coupling components. The process of fiber attachment to laser diode and welding of
various coupling components, such as lens holders, fiber ferrule and welding clips have been performed in what is so called
active alignment process, where the system continues measuring the coupled power during the process of coupling and
welding of coupling components in their holder to each other and to the main substrate. It has been found that double ball
lenses coupling scheme is efficient and more effective for mode matching of highly elliptical (large divergence ratio) laser
diode mode field with the circular mode field of a single mode fiber, whereas for small divergence ratios the single ball lens
is adequate.
A laser diode transmitter packaged in a butterfly module is coupled into a single mode fiber using double small ball
lenses. The process of alignment and fixing of all the components inside the module is performed in an active alignment
procedure, where the laser diode is powered and the output power is continuously measured during the alignment process
of all coupling components to determine the optimum positions for maximum coupling efficiency and then fixed in their
holders and to the main substrate by laser welding technique using dual beam Nd:YAG laser welding. The double ball
lenses coupling scheme found to be very effective in mode matching between laser diode and single mode fiber. The
axial, lateral and angular 1dB misalignment tolerances are enhanced for the transformed laser mode field radii in both X
and Y directions. The experimentally measured coupling efficiency of the proposed coupling system was around 75%
with a relaxed working distance (separation of the coupling system from the fiber tip) in the range of (2-4mm) by
optimizing the separation between the two lenses as well as the separation between the first lens and the facet of the laser
diode. The experimental results match very well with those obtained theoretically by employing ABCD ray tracing
matrix.
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