We experimentally demonstrated a temperature sensor by selectively infiltrating refractive index liquid (RIL) in the central air hole of a twin-core photonic crystal fiber (PCF). The selective liquid infiltration was realized by putting the PCF in the bulk liquid with its central air hole open for liquid infiltration using capillary effect. The rest of the air holes were covered by UV glue. The three-dimensional stage was used to translate the PCF, and a tapered SMF was used to transfer the UV glue to cover the air holes under the microscope. After UV glue was solidified by exposing the fiber end under the UV light, the PCF end was dipped into the RIL to fill the central air hole by capillary effect. Due to the large thermos-optic coefficient of the RIL, the RIL filled air channel would act as a liquid core whose core modes would be highly dependent on the ambient temperature. The core modes of the RIL filled core would be phase matched to the fundamental mode of the two solid cores. Therefore, the phase matching wavelengths for the mode coupling among the two solid cores of PCF and the liquid core were highly temperature sensitive. The resonant dips in the transmission spectrum were measured to estimate the temperature sensitivity. The experiment used a commercially available twin core PCF, and blocked all but the central airhole at one of the ends facets by UV glue (NOA81, Norland), the remaining open holes are infiltrated over a length of 10 cm by capillary force with fluid (Cargille Laboratories Inc. index-matching fluid, series A) that possesses a refractive index of 1.46 at 589.3nm, 25°C, and the thermal coefficient is – 0.000389 RIU/°C, which is around 10 times of that coefficient of silica. Any temperature induced changes will have an influence on the propagation properties because of the highly temperature response of the refractive index of the fluid. With a fiber cleaver, a 1.8 cm long PCF was then cut from the longer length of the partially liquid filled twin core PCF and then fusion spliced with SMFs at both ends to observe its transmission spectrum when the sample is heated. When the temperature increase to around 54°C, the liquid RI drops quickly to match that of silica, and a three parallel waveguide structure is formed, in which the central liquid waveguide have the same index value with the two solid core. Because of the small separation between adjacent waveguides, a strong mode-field overlap occurs, which leads to a significant enhancement of the coupling coefficient, therefore, light energy can be easily transferred between two solid cores and the liquid rod in a short coupling length. Thus, the transmission spectrum of the device contain two sets of interference fringe pattern, the large spectrum envelope originated from the interference between the three eigenmodes generated by three-parallel waveguide structure based on the mode coupling theory, and fine interference fringes generated by the interference between the higher order modes in one core. By tracking the dip wavelength shift of the large spectrum envelope, the sensor exhibited a high temperature sensitivity of up to 37.011 nm/°C within the temperature range from 53.8°C to 55°C due to the satisfaction of phase match condition, and maintain a high sensitivity of 19.681 nm/°C from 55°C to 58.2°C, which is benefit from the high thermal optic coefficient of the selectively filled liquid in the twin core PCF.
Second harmonic generation (SHG) is a ubiquitous technique for extending the spectral coverage of laser sources into regions that would otherwise be technologically challenging to access. SHG schemes typically rely on the use of bulk optical components, resulting in systems with large footprints requiring precise optical alignment. Integration of the SHG components into a single unit facilitates the implementation of compact, robust and turn-key sources, suitable for applications in biophotonic imaging, amongst others. We report on the development of fiber-coupled frequency doubling modules and their application to novel fiberintegrated picosecond pulse sources in the visible and near-visible. The modules employ a simple, single-pass configuration using a periodically-poled lithium niobate (PPLN) crystal as the nonlinear conversion medium. They are readily adaptable for different fiber pump laser configurations and are configurable with either fiber-coupled or collimated free-space outputs. Two sources using the modules are presented, operating at 780 nm and 560 nm. The 780 nm source utilizes an erbium master oscillator power fiber amplifier (MOPFA) scheme. SHG was performed in a 35 mm long crystal, generating 3.5 W of 780 nm radiation with a pulse duration of 410 ps at 50 MHz and conversion efficiencies exceeding 20%. Results of this source being used for parametric wavelength conversion in photonic crystal fiber are discussed. The 560 nm source was based on SHG of a Raman amplified CW diode pumped by a pulsed ytterbium-fiber MOPFA. This source generated 450 mW of average power with conversion efficiencies greater than 20%.
The exploitations of air holes in optical fiber design have been receiving growing research interest since the first
photonic crystal fiber (PCF) was demonstrated. Many peculiar optical properties are achievable with the flexible control
of the geometry of the air holes in the microstructured cladding. Different from the complex geometry of microstructured
cladding in the holey PCF, hole-assisted lightguide fiber (HALF) is based on conventional optical fiber design and
therefore guides light by total internal reflection. The existence of the assisting air holes in the cladding helps to tailor the
optical properties of the fiber. In this work, the dispersion tailoring is demonstrated by varying the structural parameters
and material properties of the fiber. Additional tunability is achieved by infiltrating substance with tunable refractive
index into the assisting holes.
Microwave signals distributed over optical fibre are of great interest for many applications. There are many
advantages of all-optical microwave filters for the direct processing of microwave signals in the optical domain, such as,
large time-bandwidth products, insensitivity to electromagnetic interference, low loss, and lightweight. A number of low
pass photonic microwave filters have been reported, where it is required to achieve optically incoherent summing of two
light beams. To overcome the optical coherence problem, either a laser array is used, or the coherence length of the light
source is kept smaller than the minimum delay time of the filter. Incoherent summing in bandpass filter has also been
achieved; however, they require very long length of Hi-Bi fibre.
We propose here all-optical low pass and bandpass microwave photonic filters configurations, together with their
application in a 20 km radio-over-fibre (RoF) link. The key problem when using a narrow linewidth source is the
coherent operation because of the narrow laser source. High differential group delay (DGD) will be induced by Hi-Bi
linearly chirped fibre Bragg grating (LCFBG), the optical interference is avoided because the two orthogonal state of
polarizations (SOPs). Meanwhile, the positive or negative chromatic dispersion (CD) will also be provided by the
chirped Hi-Bi LCFBG. The bandpass resonance is eliminated by the use of phase modulation. The CD value also can be
compensated or increased by the chirped LCFBG in the RoF link for both low pass and bandpass filters. Measured
results agree well with the theoretical results.
A full-vectorial analysis of photonic crystal fibers based on a compact two-dimensional finite-difference
time-domain method (C2D-FDTD) is presented. The model with material dispersion incorporation is
formulated and validated. The Sellmeier equation is implicitly included into the model to account for
the material dispersion of silica. In this paper we use a formulation of Maxwell's curl equations by
electric flux density and magnetic field intensity, with auxiliary differential equations; and we
demonstrate the flexibility and robustness of this approach in treating general material in PCF. We
have good agreement with multipole method.
Distributed sensors, based on Brillouin effect in the optical fiber, provide an excellent method for measuring temperature
and strain over long distances. There are two types of such sensors. The first type is based on spontaneous Brillouin
scattering, and is called Brillouin optical time domain reflectometer (BOTDR). It measures the Brillouin frequency shift
or Brillouin power or Brillouin gain bandwidth to get the temperature and strain information. The second type of sensor
is based on stimulated Brillouin amplification. It is called Brillouin optical time domain analyzer(BOTDA). Normally, it
uses one laser at each fiber ends, one as pump and the other as a probe light. The probe light will experience Brillouin
amplification. Through the analysis of Brillouin gain spectrum (BGS), we can get the temperature and strain information.
Both the two types of sensors are attracting attention all over the world, and temperature resolution of less than 1 degree
and strain resolution up to 5 με was reported. The fiber distances of up to 150km was presented while other papers
reported a spatial resolution of the order of 1cm with frequency domain techniques or correlation techniques. We
proposed and analyzed our design, it is an improvement of BOTDA with a single end laser, which make it easy to
implement in field. Through simulations, optimized launch power has been found for a certain design.
The fabrication of a tunable all-solid photonic bandgap fiber coupler based on side-polishing technique is reported.
The all-solid photonic bandgap fiber is set into a silica block and then polished to access the evanescent field. The
photonic bandgap fiber coupler was assembled by mating two identical half-blocks with each other. By
longitudinally adjusting the relative position between the mated pair, the tunable coupling ratio as much as 92.5% at
1550 nm is achieved. The investigation of the spectrum properties shows that the coupler has excellent tunability
properties, for which the coupling ratio can be smoothly and continuously tuned.
We proposed flexible bandwidth control for a two-dimensional (2D) photonic crystal coupled-cavity waveguide. The 2D waveguide is designed to operate in single-mode. The bandwidth not only determines the operating frequency range of the waveguide, but also affects the group velocity of the guided modes much. Researches in enlargement and precise controlling of bandwidth are of great importance for waveguide structure design based on photonic crystals. Moreover, to keep the signal pulse shape along a single-mode waveguide, minimized group velocity within a wide bandwidth is required for the design. In our previous studies we have demonstrated controlling the upper and lower cut off frequencies of the guided band both independently and simultaneously. In this work, large bandwidth-tuning for a single-mode guided band with fixed center frequency is realized by changing two configuration parameters, namely defect radius and defect width. Plane wave expansion method is utilized for calculation. The largest bandwidth tuning range up to 50.7% of photonic bandgap (PBG) is achieved for normalized center frequency at 0.377. Furthermore, for different bandwidths, we investigate the relations of group velocities and wave vectors, which are crucial to engineer the group velocity dispersion in the waveguide. Our results demonstrate the possibility of large bandwidth tuning while single-mode operation is maintained, which could be extended to photonic crystal slab waveguide with some modifications. We believe this work will contribute to the design of integrated optical devices based on photonic crystal waveguides, such as multiplexers and de-multiplexers which can make use of the flexible bandwidth control capabilities.
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